diff --git a/.gitignore b/.gitignore index 67bc9fa6b..fe0a24d5d 100644 --- a/.gitignore +++ b/.gitignore @@ -10,6 +10,7 @@ !README.md !README.swifter !*.in +dump* !example/cleanup !example/swifter_symba_omp !Makefile diff --git a/Makefile b/Makefile index 94dfbceeb..b5fb81071 100644 --- a/Makefile +++ b/Makefile @@ -45,9 +45,11 @@ #****************************************************************************** SWIFTEST_MODULES = swiftest_globals.f90 \ + swiftest_operators.f90 \ lambda_function.f90\ + walltime_classes.f90 \ swiftest_classes.f90 \ - swiftest_operators.f90 \ + fraggle_classes.f90 \ whm_classes.f90 \ rmvs_classes.f90 \ helio_classes.f90 \ @@ -57,13 +59,13 @@ SWIFTEST_MODULES = swiftest_globals.f90 \ include Makefile.Defines -MODULES = $(SWIFTEST_MODULES) $(USER_MODULES) +MODULES = $(SWIFTEST_MODULES) $(USER_MODULES) .PHONY : all mod lib libdir drivers bin clean force % : %.f90 force - $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include $< -o $@ \ - -L$(SWIFTEST_HOME)/lib -lswiftest + $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include -I$(NETCDF_FORTRAN_HOME)/include $< -o $@ \ + -L$(SWIFTEST_HOME)/lib -lswiftest -L$(NETCDF_FORTRAN_HOME)/lib -lnetcdf -lnetcdff $(INSTALL_PROGRAM) $@ $(SWIFTEST_HOME)/bin rm -f $@ @@ -75,7 +77,7 @@ all: mod: cd $(SWIFTEST_HOME)/src/modules/; \ - $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include -c $(MODULES); \ + $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include -I$(NETCDF_FORTRAN_HOME)/include -c $(MODULES); \ $(AR) rv $(SWIFTEST_HOME)/lib/libswiftest.a *.o; \ $(INSTALL_DATA) *.mod *.smod $(SWIFTEST_HOME)/include; \ rm -f *.o *.mod *.smod @@ -91,27 +93,27 @@ lib: ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ make libdir - cd $(SWIFTEST_HOME)/src/eucl; \ + cd $(SWIFTEST_HOME)/src/fraggle; \ rm -f Makefile.Defines Makefile; \ ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ make libdir - cd $(SWIFTEST_HOME)/src/fragmentation; \ + cd $(SWIFTEST_HOME)/src/gr; \ rm -f Makefile.Defines Makefile; \ ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ make libdir - cd $(SWIFTEST_HOME)/src/gr; \ + cd $(SWIFTEST_HOME)/src/io; \ rm -f Makefile.Defines Makefile; \ ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ make libdir - cd $(SWIFTEST_HOME)/src/io; \ + cd $(SWIFTEST_HOME)/src/kick; \ rm -f Makefile.Defines Makefile; \ ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ make libdir - cd $(SWIFTEST_HOME)/src/kick; \ + cd $(SWIFTEST_HOME)/src/netcdf; \ rm -f Makefile.Defines Makefile; \ ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \ ln -s $(SWIFTEST_HOME)/Makefile .; \ @@ -173,7 +175,7 @@ lib: make libdir libdir: - $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include -c *.f90; \ + $(FORTRAN) $(FFLAGS) -I$(SWIFTEST_HOME)/include -I$(NETCDF_FORTRAN_HOME)/include -c *.f90; \ $(AR) rv $(SWIFTEST_HOME)/lib/libswiftest.a *.o *.smod; \ $(INSTALL_DATA) *.smod $(SWIFTEST_HOME)/include; \ rm -f *.o *.smod @@ -193,13 +195,13 @@ clean: cd $(SWIFTEST_HOME)/src/modules; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/discard; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/drift; rm -f Makefile.Defines Makefile *.gc* - cd $(SWIFTEST_HOME)/src/eucl; rm -f Makefile.Defines Makefile *.gc* - cd $(SWIFTEST_HOME)/src/fragmentation; rm -f Makefile.Defines Makefile *.gc* + cd $(SWIFTEST_HOME)/src/fraggle; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/gr; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/helio; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/io; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/kick; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/main; rm -f Makefile.Defines Makefile *.gc* + cd $(SWIFTEST_HOME)/src/netcdf; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/obl; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/operators; rm -f Makefile.Defines Makefile *.gc* cd $(SWIFTEST_HOME)/src/orbel; rm -f Makefile.Defines Makefile *.gc* diff --git a/Makefile.Defines b/Makefile.Defines index 820ad6d7d..36de2cdb7 100644 --- a/Makefile.Defines +++ b/Makefile.Defines @@ -51,27 +51,29 @@ ADVIXE_FLAGS = -g -O2 -qopt-report=5 -vec -vecabi=cmdtarget -simd -shared-intel VTUNE_FLAGS = -g -O2 -vec -simd -shared-intel -qopenmp -debug inline-debug-info -parallel-source-info=2 -parallel -DTBB_DEBUG -DTBB_USE_THREADING_TOOLS -qopenmp -fp-model no-except -mp1 -xhost -traceback #Be sure to set the environment variable KMP_FORKJOIN_FRAMES=1 for OpenMP debuging in vtune -IDEBUG = -O0 -nogen-interfaces -no-pie -no-ftz -fpe-all=0 -g -traceback -mp1 -fp-model strict -fpe0 -debug all -align all -pad -ip -prec-div -prec-sqrt -assume protect-parens -CB -no-wrap-margin -init=snan,arrays +IDEBUG = -O0 -init=snan,arrays -nogen-interfaces -no-pie -no-ftz -fpe-all=0 -g -traceback -mp1 -fp-model strict -fpe0 -debug all -align all -pad -ip -prec-div -prec-sqrt -assume protect-parens -CB -no-wrap-margin STRICTREAL = -fp-model strict -fp-model no-except -prec-div -prec-sqrt -assume protect-parens SIMDVEC = -simd -xhost -align all -assume contiguous_assumed_shape -vecabi=cmdtarget -prec-div -prec-sqrt -assume protect-parens -PAR = -parallel -qopenmp +PAR = -qopenmp #-parallel #Something goes wrong in SyMBA at the moment with auto-paralellization enabled HEAPARR = -heap-arrays 1048576 -OPTIMIZE = -qopt-report=5 +OPTREPORT = -qopt-report=5 +IPRODUCTION = -init=snan,arrays -no-wrap-margin -O3 $(STRICTREAL) $(PAR) $(SIMDVEC) $(HEAPARR) #gfortran flags -GDEBUG = -g -O0 -fbacktrace -fbounds-check -GPRODUCTION = -O3 -GPAR = -fopenmp -ftree-parallelize-loops=4 -GMEM = -fsanitize=undefined -fsanitize=address -fsanitize=leak +GDEBUG = -g -Og -fbacktrace -fbounds-check -ffree-line-length-none +GPAR = -fopenmp #-ftree-parallelize-loops=4 +GMEM = -fsanitize-address-use-after-scope -fstack-check -fsanitize=bounds-strict -fsanitize=undefined -fsanitize=signed-integer-overflow -fsanitize=object-size -fstack-protector-all GWARNINGS = -Wall -Warray-bounds -Wimplicit-interface -Wextra -Warray-temporaries +GPRODUCTION = -O3 -ffree-line-length-none $(GPAR) -#FFLAGS = $(IDEBUG) $(HEAPARR) -FFLAGS = -init=snan,arrays -no-wrap-margin -O3 $(STRICTREAL) $(SIMDVEC) $(PAR) +#FFLAGS = $(IDEBUG) $(HEAPARR) $(SIMDVEC) $(PAR) +FFLAGS = $(IPRODUCTION) $(OPTREPORT) FORTRAN = ifort #AR = xiar #FORTRAN = gfortran -#FFLAGS = -ffree-line-length-none $(GDEBUG) #$(GMEM) +#FFLAGS = $(GDEBUG) $(GMEM) $(GPAR) +#FFLAGS = $(GPRODUCTION) -g -fbacktrace #-fcheck=all #-Wall AR = ar # DO NOT include in CFLAGS the "-c" option to compile object only diff --git a/examples/helio_gr_test/cb.swiftest.in b/examples/helio_gr_test/cb.swiftest.in index e4a010b1e..64406c4cf 100644 --- a/examples/helio_gr_test/cb.swiftest.in +++ b/examples/helio_gr_test/cb.swiftest.in @@ -1,4 +1,4 @@ -0 +Sun 39.476926408897626 0.004650467260962157 4.7535806948127355e-12 diff --git a/examples/helio_gr_test/init_cond.py b/examples/helio_gr_test/init_cond.py index 5b378da74..e4351de42 100755 --- a/examples/helio_gr_test/init_cond.py +++ b/examples/helio_gr_test/init_cond.py @@ -5,8 +5,7 @@ sim.param['PL_IN'] = "pl.swiftest.in" sim.param['TP_IN'] = "tp.swiftest.in" sim.param['CB_IN'] = "cb.swiftest.in" -sim.param['BIN_OUT'] = "bin.swiftest.dat" -sim.param['ENC_OUT'] = "enc.swiftest.dat" +sim.param['BIN_OUT'] = "bin.swiftest.nc" sim.param['MU2KG'] = swiftest.MSun sim.param['TU2S'] = swiftest.YR2S @@ -22,9 +21,11 @@ sim.param['CHK_RMIN'] = swiftest.RSun / swiftest.AU2M sim.param['CHK_RMAX'] = 1000.0 sim.param['CHK_EJECT'] = 1000.0 -sim.param['OUT_FORM'] = "EL" sim.param['OUT_STAT'] = "UNKNOWN" -sim.param['RHILL_PRESENT'] = "NO" +sim.param['IN_FORM'] = "EL" +sim.param['OUT_FORM'] = "XVEL" +sim.param['OUT_TYPE'] = "NETCDF_DOUBLE" +sim.param['RHILL_PRESENT'] = "YES" sim.param['GR'] = 'YES' bodyid = { diff --git a/examples/helio_gr_test/param.swifter.in b/examples/helio_gr_test/param.swifter.in index acca6f7aa..14a2e67ab 100644 --- a/examples/helio_gr_test/param.swifter.in +++ b/examples/helio_gr_test/param.swifter.in @@ -4,24 +4,24 @@ TSTOP 1000.0 DT 0.0006844626967830253 ISTEP_OUT 1461 ISTEP_DUMP 1461 -OUT_FORM EL -OUT_TYPE REAL8 +OUT_FORM XVEL +OUT_TYPE NETCDF_DOUBLE OUT_STAT UNKNOWN IN_TYPE ASCII PL_IN pl.swifter.in TP_IN tp.swifter.in BIN_OUT bin.swifter.dat -ENC_OUT enc.swifter.dat CHK_QMIN 0.004650467260962157 CHK_RMIN 0.004650467260962157 CHK_RMAX 1000.0 CHK_EJECT 1000.0 CHK_QMIN_COORD HELIO CHK_QMIN_RANGE 0.004650467260962157 1000.0 +ENC_OUT enc.swifter.dat EXTRA_FORCE NO BIG_DISCARD NO CHK_CLOSE YES -RHILL_PRESENT NO +RHILL_PRESENT YES C 63241.07708426628 J2 4.7535806948127355e-12 J4 -2.2473967953572827e-18 diff --git a/examples/helio_gr_test/param.swiftest.in b/examples/helio_gr_test/param.swiftest.in index f5a748693..06cd551b5 100644 --- a/examples/helio_gr_test/param.swiftest.in +++ b/examples/helio_gr_test/param.swiftest.in @@ -4,15 +4,14 @@ TSTOP 1000.0 DT 0.0006844626967830253 ISTEP_OUT 1461 ISTEP_DUMP 1461 -OUT_FORM EL -OUT_TYPE REAL8 +OUT_FORM XVEL +OUT_TYPE NETCDF_DOUBLE OUT_STAT UNKNOWN IN_TYPE ASCII PL_IN pl.swiftest.in TP_IN tp.swiftest.in CB_IN cb.swiftest.in -BIN_OUT bin.swiftest.dat -ENC_OUT enc.swiftest.dat +BIN_OUT bin.swiftest.nc CHK_QMIN 0.004650467260962157 CHK_RMIN 0.004650467260962157 CHK_RMAX 1000.0 @@ -22,15 +21,15 @@ CHK_QMIN_RANGE 0.004650467260962157 1000.0 MU2KG 1.988409870698051e+30 TU2S 31557600.0 DU2M 149597870700.0 +IN_FORM EL +ENC_OUT enc.dat EXTRA_FORCE NO +DISCARD_OUT discard.out BIG_DISCARD NO CHK_CLOSE YES -RHILL_PRESENT NO +RHILL_PRESENT YES FRAGMENTATION NO ROTATION NO TIDES NO ENERGY NO GR YES -YARKOVSKY NO -YORP NO -MTINY 0.0 diff --git a/examples/helio_gr_test/pl.swifter.in b/examples/helio_gr_test/pl.swifter.in index f39e7af56..9add1dc1a 100644 --- a/examples/helio_gr_test/pl.swifter.in +++ b/examples/helio_gr_test/pl.swifter.in @@ -1,36 +1,36 @@ 9 -0 39.476926408897625196 +0 39.476926408897626 0.0 0.0 0.0 0.0 0.0 0.0 -1 6.5537098095653139645e-06 +1 6.5537098095653139645e-06 0.001475131156288637831 1.6306381826061645943e-05 --0.30949970210807342674 0.1619004125820537876 0.041620272188990829754 --6.8742992150644793847 -8.672423996611946485 -0.078109307586001638286 -2 9.663313399581537916e-05 +-0.0361820239646683528 -0.46276010580341980782 -0.034496398006472611675 +8.183688458560222766 -0.27616682338432374386 -0.7732476400340904169 +2 9.663313399581537916e-05 0.0067590747715647875607 4.0453784346544178454e-05 --0.5567137338251560985 -0.46074173273652380134 0.02580196630219121906 -4.6580776303108450487 -5.726444072926637749 -0.3473859047161406309 -3 0.000120026935827952453094 +0.04707194870345993154 -0.7255425078625500346 -0.012673782840571969424 +7.3226765098927520106 0.45143529808423807744 -0.4163607714267330732 +3 0.000120026935827952453094 0.01004493295891520948 4.25875607065040958e-05 -0.6978790186886838498 -0.73607603319120218366 3.261671020506711323e-05 -4.4579240279134950613 4.300011122687349501 -0.00022055769049333364448 -4 1.2739802010675941456e-05 +0.9784182446151709067 -0.2394545623617302943 7.8432240502479141865e-06 +1.3916805835822199726 6.0802455505175572043 -0.00029695052429473289775 +4 1.2739802010675941456e-05 0.007246527815634877893 2.265740805092889601e-05 --1.617661473167097963 0.38314370807747849534 0.04771055403546069218 --0.98751874613118001086 -4.5371239937302254657 -0.07086074102213555221 -5 0.037692251088985676735 +-1.64827450584581503 -0.04818173529735803734 0.039422108862210397673 +0.3393812176064170994 -4.672429323734897043 -0.1062469093563351878 +5 0.037692251088985676735 0.3552712221482522291 0.00046732617030490929307 -4.1527454588897487753 -2.8347492039446908763 -0.081136554176388195336 -1.5225069137843642898 2.4087104911325327961 -0.044067446366273183833 -6 0.011285899820091272997 +4.2888079225575648223 -2.6068082746690541818 -0.08512743586621877856 +1.4000629754656241179 2.4876377693334669565 -0.04165606656604725836 +6 0.011285899820091272997 0.4376655756331854547 0.00038925687730393611812 -6.39471595410062843 -7.621162747287802297 -0.121992225877669294154 -1.4493167787574136286 1.3075474785896286071 -0.08039429377859412155 -7 0.0017236589478267730203 +6.528501376442308768 -7.4981197287393284157 -0.12945412016904539465 +1.4250071771025915456 1.33599992135721594 -0.07992159012428249671 +7 0.0017236589478267730203 0.46970222329693796102 0.00016953449859497231466 -14.793135356927480828 13.074218343364380601 -0.14311846037737518955 --0.9605086875596024784 1.0118431725941020164 0.016148779866732710198 -8 0.0020336100526728302319 +14.703390521074780395 13.168120788311910019 -0.14161196287363458923 +-0.96768368440931795183 1.0056701102995595347 0.01621895610074016891 +8 0.0020336100526728302319 0.78148373992374883156 0.000164587904124493665 -29.568629894896030663 -4.5543028991960081697 -0.58771107137394917874 -0.16867624969736024011 1.1427992197933557251 -0.027387722828706092838 +29.584136736556288838 -4.4478894754775319953 -0.5902566603324214123 +0.16448791459483679965 1.1435219564135608914 -0.027304639012640681262 diff --git a/examples/helio_gr_test/pl.swiftest.in b/examples/helio_gr_test/pl.swiftest.in index b624d25ba..cd6a82534 100644 --- a/examples/helio_gr_test/pl.swiftest.in +++ b/examples/helio_gr_test/pl.swiftest.in @@ -1,33 +1,33 @@ 8 -1 6.5537098095653139645e-06 +Mercury 6.5537098095653139645e-06 0.001475131156288637831 1.6306381826061645943e-05 --0.30949970210807342674 0.1619004125820537876 0.041620272188990829754 --6.8742992150644793847 -8.672423996611946485 -0.078109307586001638286 -2 9.663313399581537916e-05 +0.38709993253896590737 0.20562614632859010921 7.0036272314159866426 +48.303648911363737284 29.187750438580689405 192.22398026813181104 +Venus 9.663313399581537916e-05 0.0067590747715647875607 4.0453784346544178454e-05 --0.5567137338251560985 -0.46074173273652380134 0.02580196630219121906 -4.6580776303108450487 -5.726444072926637749 -0.3473859047161406309 -3 0.000120026935827952453094 +0.7233249152313999675 0.006782779674600277614 3.3945084679511872139 +76.62172192899298295 55.11871576732421829 141.51944714681908977 +Earth 0.000120026935827952453094 0.01004493295891520948 4.25875607065040958e-05 -0.6978790186886838498 -0.73607603319120218366 3.261671020506711323e-05 -4.4579240279134950613 4.300011122687349501 -0.00022055769049333364448 -4 1.2739802010675941456e-05 +1.0000207198983319667 0.01667731166077134064 0.0027576432734417160447 +175.55813761562768605 287.40166532678227895 245.00485341438161413 +Mars 1.2739802010675941456e-05 0.007246527815634877893 2.265740805092889601e-05 --1.617661473167097963 0.38314370807747849534 0.04771055403546069218 --0.98751874613118001086 -4.5371239937302254657 -0.07086074102213555221 -5 0.037692251088985676735 +1.5236922769560579116 0.093361659829406723476 1.8479133359077690724 +49.490611477105659333 286.70751815915190264 210.36775515565921069 +Jupiter 0.037692251088985676735 0.3552712221482522291 0.00046732617030490929307 -4.1527454588897487753 -2.8347492039446908763 -0.081136554176388195336 -1.5225069137843642898 2.4087104911325327961 -0.044067446366273183833 -6 0.011285899820091272997 +5.203523661489898977 0.04851833897394460665 1.3035686835324369337 +100.51671881401649955 273.38319313278452682 318.65986979714938343 +Saturn 0.011285899820091272997 0.4376655756331854547 0.00038925687730393611812 -6.39471595410062843 -7.621162747287802297 -0.121992225877669294154 -1.4493167787574136286 1.3075474785896286071 -0.08039429377859412155 -7 0.0017236589478267730203 +9.581904852310625387 0.052236260603057811658 2.486258128114103183 +113.595257336893098454 335.64742317800698856 225.92836894588160135 +Uranus 0.0017236589478267730203 0.46970222329693796102 0.00016953449859497231466 -14.793135356927480828 13.074218343364380601 -0.14311846037737518955 --0.9605086875596024784 1.0118431725941020164 0.016148779866732710198 -8 0.0020336100526728302319 +19.238019712529130345 0.0442880601027018303 0.770350326736000679 +74.09520891350530292 95.7524345508490029 236.07863258800219342 +Neptune 0.0020336100526728302319 0.78148373992374883156 0.000164587904124493665 -29.568629894896030663 -4.5543028991960081697 -0.58771107137394917874 -0.16867624969736024011 1.1427992197933557251 -0.027387722828706092838 +30.291369954344219195 0.013531244039650480379 1.7689741418447819665 +131.74449502957048708 245.89296040993210113 334.5035290478779757 diff --git a/examples/in_form_el/cb.in b/examples/in_form_el/cb.in new file mode 100644 index 000000000..673a79459 --- /dev/null +++ b/examples/in_form_el/cb.in @@ -0,0 +1,5 @@ +0 +0.0002959122081920778 +0.004650467260962157 +4.7535806948127355e-12 +-2.2473967953572827e-18 diff --git a/examples/in_form_el/param.in b/examples/in_form_el/param.in new file mode 100644 index 000000000..409cd2d2b --- /dev/null +++ b/examples/in_form_el/param.in @@ -0,0 +1,35 @@ +! VERSION Swiftest parameter input from file param.in +T0 0.0 +TSTOP 365250000000.0 +DT 5.0 +ISTEP_OUT 7305000 +ISTEP_DUMP 7305000 +OUT_FORM EL +OUT_TYPE REAL8 +OUT_STAT REPLACE +IN_TYPE ASCII +PL_IN pl.in +TP_IN tp.in +CB_IN cb.in +BIN_OUT bin.dat +CHK_QMIN 0.004650467260962157 +CHK_RMIN 0.004650467260962157 +CHK_RMAX 1000.0 +CHK_EJECT 1000.0 +CHK_QMIN_COORD HELIO +CHK_QMIN_RANGE 0.004650467260962157 1000.0 +MU2KG 1.988409870698051e+30 +TU2S 86400.0 +DU2M 149597870700.0 +IN_FORM EL +ENC_OUT enc.dat +EXTRA_FORCE NO +DISCARD_OUT discard.out +BIG_DISCARD NO +CHK_CLOSE YES +RHILL_PRESENT YES +FRAGMENTATION NO +ROTATION NO +TIDES NO +ENERGY NO +GR YES diff --git a/examples/in_form_el/pl.in b/examples/in_form_el/pl.in new file mode 100644 index 000000000..55748b408 --- /dev/null +++ b/examples/in_form_el/pl.in @@ -0,0 +1,33 @@ +8 +1 4.9125474498983625e-11 0.0014751256791533402 +1.6306381826061646e-05 +0.38710383731080894 0.24071190040066506 8.640070276952633 +30.683987164281632 57.949871930463694 151.08868778597147 +2 7.243452483873647e-10 0.0067591154147628296 +4.0453784346544176e-05 +0.7233315774753523 0.02498272794314777 2.4772002857938187 +125.76075677093282 6.742571718202682 350.2972657114627 +3 8.997011382166019e-10 0.010044745408888887 +4.25875607065041e-05 +0.9999904186618421 0.05232751342856539 2.0722848768764717 +113.84624589363827 312.12453079628943 148.9860363695549 +4 9.549535102761465e-11 0.007246758104365299 +2.2657408050928896e-05 +1.5236293140305446 0.005382832120155795 4.468216946001687 +325.6098790099478 152.40711385323957 110.04936074450407 +5 2.825345908631355e-07 0.3552714410085414 +0.0004673261703049093 +5.203095539549931 0.03063821583296288 1.3661365597246853 +113.82182400586191 303.52091573107697 96.03226696213453 +6 8.459715183006416e-08 0.43765112940564116 +0.00038925687730393614 +9.579329287028964 0.08182512713593486 2.54624964218005 +100.32672664745415 306.8523855342038 64.14978871000847 +7 1.2920249163736674e-08 0.4695173932519177 +0.00016953449859497232 +19.185526866180975 0.02725895554029442 0.6468816262831063 +75.84341829565291 203.1828812930829 337.91763726094723 +8 1.5243589003230834e-08 0.7812638143548571 +0.00016458790412449367 +30.033406636357004 0.014808837377897958 1.0172902231424474 +112.31047122167676 61.6982073585126 219.66063286932612 diff --git a/examples/in_form_el/tp.in b/examples/in_form_el/tp.in new file mode 100644 index 000000000..48e97fb82 --- /dev/null +++ b/examples/in_form_el/tp.in @@ -0,0 +1,76 @@ +25 +1030101 +1.9298376430729873 0.012639757841142886 24.991702977377773 +341.74785371597466 248.1210122966632 133.62225322652563 +1030102 +1.9576788467130908 0.027970945719088838 25.55968189226752 +168.9126943096874 174.5978360268346 251.14179333855816 +1030103 +1.967626111006107 0.09226955476091864 1.5279774530000956 +343.6507149897438 15.943105536008861 203.03043240705532 +1030104 +1.9481905063928624 0.0011928078627614026 13.712706682327513 +65.70102045298484 272.5349689212673 248.3878548054673 +1030105 +1.9770133412534745 0.07760502570359305 21.113956523745326 +352.7420976555242 265.31463697173825 90.20915048805514 +1030106 +1.9218154288668319 0.024539743705313734 6.3122997131518 +96.26526838131817 245.40058043017729 203.1458881543752 +1030107 +1.8804043534140047 0.051960914508786316 5.641080857843637 +135.37074231372475 310.57579433118855 92.01889766237802 +1030108 +1.905574620628057 0.0094526649542939 27.795518144975087 +257.055868633706 262.18164024081847 174.33454380356292 +1030109 +1.9610371451706512 0.0642394856575368 11.238178270217231 +155.06613544539204 179.7982091248266 227.65351567825778 +1030110 +1.8442099887042422 0.06774466132861966 7.7755827872476635 +53.89722157548661 231.27772356054047 224.74925586092095 +1030111 +1.918614204096997 0.09311188233380624 22.656238093717935 +8.91787503082778 121.09392635435141 61.064615587866086 +1030112 +1.846083421031052 0.058817512099736215 23.17733139808657 +204.2210767808533 325.0096873835248 80.8104389106319 +1030113 +1.877211316979287 0.09545803603787674 22.75125883423326 +338.55088656488704 260.97440743659024 358.27993618149003 +1030114 +1.847699999560908 0.04422349734135026 24.400107433270254 +175.41066398268853 271.9213024922804 40.10860995923193 +1030115 +1.9693855972875431 0.01087613268562867 18.3688586644925 +288.07225817085316 351.2861239674453 138.17614312177193 +1030116 +1.8499142747340205 0.05785154439430367 18.680424125046468 +170.34777680935684 121.2501486818594 116.63207933400314 +1030117 +1.8484833703421926 0.027361686628703055 12.35340287511839 +77.72361263316543 170.96254103643864 153.80655599509745 +1030118 +1.8844066519945433 0.012253504795668403 28.11812027401767 +5.816089316051807 234.40531004184038 284.0432510837761 +1030119 +1.8321110668963587 0.05520820027904241 4.246848772229706 +195.98962278787414 196.26877791689589 296.01468603344676 +1030120 +1.9298252957677076 0.04051603959563857 11.38835718089586 +14.020062127093711 350.7131191785245 61.91415736777295 +1030121 +1.8296584872076656 0.02265081514507832 19.242848763922552 +170.21169721403766 255.88594273947075 131.4644380844818 +1030122 +1.8699958208259342 0.08248881864547655 6.775274873263883 +131.47697608382563 36.70815817760613 166.48187957273242 +1030123 +1.8427387543178881 0.07305783679736073 5.034586865380743 +311.1450141807796 214.40263993828856 332.6408661254218 +1030124 +1.8567511528637752 0.014548178017731906 8.946207161705699 +27.813385444122652 111.5675183218652 201.4816583454089 +1030125 +1.8846946839402372 0.06619567127431686 13.271555732235106 +271.1533808977903 174.59924852630596 257.0822687250529 diff --git a/examples/rmvs_swifter_comparison/1pl_1tp_encounter/init_cond.py b/examples/rmvs_swifter_comparison/1pl_1tp_encounter/init_cond.py index a700466b1..f17e000fa 100755 --- a/examples/rmvs_swifter_comparison/1pl_1tp_encounter/init_cond.py +++ b/examples/rmvs_swifter_comparison/1pl_1tp_encounter/init_cond.py @@ -55,7 +55,7 @@ p_tp = np.array([atp, 0.0, 0.0], dtype=np.double) v_tp = np.array([0.0, vtp, 0.0], dtype=np.double) -Rhill = np.double(apl * 0.0100447248332378922085) +rhill = np.double(apl * 0.0100447248332378922085) #Make Swifter files plfile = open(swifter_pl, 'w') @@ -63,7 +63,7 @@ print(1,GMSun,file=plfile) print('0.0 0.0 0.0',file=plfile) print('0.0 0.0 0.0',file=plfile) -print(plid,"{:.23g}".format(Gmass),Rhill, file=plfile) +print(plid,"{:.23g}".format(Gmass),rhill, file=plfile) print(radius, file=plfile) print(*p_pl, file=plfile) print(*v_pl, file=plfile) @@ -126,7 +126,7 @@ plfile.write_record(v_pl[1]) plfile.write_record(v_pl[2]) plfile.write_record(Gmass) -plfile.write_record(Rhill) +plfile.write_record(rhill) plfile.write_record(radius) plfile.close() tpfile = FortranFile(swiftest_tp, 'w') diff --git a/examples/rmvs_swifter_comparison/1pl_1tp_encounter/swiftest_vs_swifter.ipynb b/examples/rmvs_swifter_comparison/1pl_1tp_encounter/swiftest_vs_swifter.ipynb index 20122244c..aa7e8e5e3 100644 --- a/examples/rmvs_swifter_comparison/1pl_1tp_encounter/swiftest_vs_swifter.ipynb +++ b/examples/rmvs_swifter_comparison/1pl_1tp_encounter/swiftest_vs_swifter.ipynb @@ -81,8 +81,8 @@ { "data": { "text/plain": [ - "[,\n", - " ]" + "[,\n", + " ]" ] }, "execution_count": 6, diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/init_cond.py b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/init_cond.py index 49d017b86..5fc0ef7d0 100755 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/init_cond.py +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/init_cond.py @@ -19,12 +19,13 @@ swiftest_cb = "cb.swiftest.in" swiftest_bin = "bin.swiftest.dat" swiftest_enc = "enc.swiftest.dat" +swiftest_disc = "discard.swiftest.out" sim = swiftest.Simulation() sim.param['T0'] = 0.0 sim.param['DT'] = 1.0 -sim.param['TSTOP'] = 365.25e1 +sim.param['TSTOP'] = 365.25e2 sim.param['ISTEP_OUT'] = 10 sim.param['ISTEP_DUMP'] = 10 sim.param['CHK_QMIN_COORD'] = "HELIO" @@ -83,16 +84,16 @@ for i in pl.id: pli = pl.sel(id=i) - rstart = 2 * np.double(pli['Radius']) # Start the test particles at a multiple of the planet radius away - vstart = 1.5 * np.sqrt(2 * np.double(pli['Mass']) / rstart) # Start the test particle velocities at a multiple of the escape speed + rstart = 2 * np.double(pli['radius']) # Start the test particles at a multiple of the planet radius away + vstart = 1.5 * np.sqrt(2 * np.double(pli['Gmass']) / rstart) # Start the test particle velocities at a multiple of the escape speed xvstart = np.array([rstart / np.sqrt(2.0), rstart / np.sqrt(2.0), 0.0, vstart, 0.0, 0.0]) # The positions and velocities of each pair of test particles will be in reference to a planet - plvec = np.array([np.double(pli['px']), - np.double(pli['py']), - np.double(pli['pz']), - np.double(pli['vx']), - np.double(pli['vy']), - np.double(pli['vz'])]) + plvec = np.array([np.double(pli['xhx']), + np.double(pli['xhy']), + np.double(pli['xhz']), + np.double(pli['vhx']), + np.double(pli['vhy']), + np.double(pli['vhz'])]) tpxv1 = plvec + xvstart tpxv2 = plvec - xvstart p1.append(tpxv1[0]) @@ -124,6 +125,7 @@ sim.param['CB_IN'] = swiftest_cb sim.param['BIN_OUT'] = swiftest_bin sim.param['ENC_OUT'] = swiftest_enc +sim.param['DISCARD_OUT'] = swiftest_disc sim.save(swiftest_input) sim.param['PL_IN'] = swifter_pl diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swifter.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swifter.in index 36dd2060f..acd0bd0ce 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swifter.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swifter.in @@ -1,9 +1,9 @@ ! VERSION Swifter parameter file converted from Swiftest T0 0.0 -TSTOP 3652.5 +TSTOP 9500.0 DT 1.0 -ISTEP_OUT 10 -ISTEP_DUMP 10 +ISTEP_OUT 100 +ISTEP_DUMP 100 OUT_FORM XV OUT_TYPE REAL8 OUT_STAT UNKNOWN @@ -11,13 +11,13 @@ IN_TYPE ASCII PL_IN pl.swifter.in TP_IN tp.in BIN_OUT bin.swifter.dat -ENC_OUT enc.swifter.dat CHK_QMIN 0.004650467260962157 CHK_RMIN 0.004650467260962157 CHK_RMAX 1000.0 CHK_EJECT 1000.0 CHK_QMIN_COORD HELIO CHK_QMIN_RANGE 0.004650467260962157 1000.0 +ENC_OUT enc.swifter.dat EXTRA_FORCE NO BIG_DISCARD NO CHK_CLOSE YES diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swiftest.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swiftest.in index b08b66850..f924ebb95 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swiftest.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/param.swiftest.in @@ -1,9 +1,9 @@ ! VERSION Swiftest parameter input T0 0.0 -TSTOP 3652.5 +TSTOP 9500.0 DT 1.0 -ISTEP_OUT 10 -ISTEP_DUMP 10 +ISTEP_OUT 100 +ISTEP_DUMP 100 OUT_FORM XV OUT_TYPE REAL8 OUT_STAT UNKNOWN @@ -12,7 +12,6 @@ PL_IN pl.swiftest.in TP_IN tp.in CB_IN cb.swiftest.in BIN_OUT bin.swiftest.dat -ENC_OUT enc.swiftest.dat CHK_QMIN 0.004650467260962157 CHK_RMIN 0.004650467260962157 CHK_RMAX 1000.0 @@ -22,7 +21,9 @@ CHK_QMIN_RANGE 0.004650467260962157 1000.0 MU2KG 1.988409870698051e+30 TU2S 86400 DU2M 149597870700.0 +ENC_OUT enc.swiftest.dat EXTRA_FORCE NO +DISCARD_OUT discard.swiftest.out BIG_DISCARD NO CHK_CLOSE YES RHILL_PRESENT YES @@ -31,6 +32,3 @@ ROTATION NO TIDES NO ENERGY NO GR NO -YARKOVSKY NO -YORP NO -MTINY 0.0 diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.in index 207dd84f6..e506d4743 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.in @@ -1,33 +1,33 @@ 8 -1 4.9125474498983623693e-11 0.001475124456355905224 +1 4.9125474498983623693e-11 0.0014751244935834097723 1.6306381826061645943e-05 --0.30949970210807342674 0.1619004125820537876 0.041620272188990829754 --0.018820805516945871005 -0.023743802865467341506 -0.00021385162925667799668 -2 7.243452483873646905e-10 0.006759069616556246028 +-0.37723213134178928962 0.033583006382262102496 0.037347605390151236704 +-0.008342765357522348782 -0.026815373891535949219 -0.0014259978126226569104 +2 7.243452483873646905e-10 0.006759064884572926305 4.0453784346544178454e-05 --0.5567137338251560985 -0.46074173273652380134 0.02580196630219121906 -0.012753121506668980284 -0.015678149412530151263 -0.0009510907726656827677 -3 8.9970113821660187435e-10 0.010044908171483009529 +-0.48772324783973242113 -0.53438159383885197595 0.020810210727290629623 +0.014797158412775200664 -0.013730742274988789325 -0.0010423161661001279551 +3 8.9970113821660187435e-10 0.01004492566381686821 4.25875607065040958e-05 -0.6978790186886838498 -0.73607603319120218366 3.261671020506711323e-05 -0.012205130808798069983 0.0117727888369263504476 -6.0385404652521189453e-07 -4 9.549535102761465607e-11 0.0072466797341124641736 +0.75635861236241797023 -0.674672320414933413 2.9482164814591560215e-05 +0.0111724732704936106226 0.0127745538308708106445 -6.4922715710692383536e-07 +4 9.549535102761465607e-11 0.007246661019460395855 2.265740805092889601e-05 --1.617661473167097963 0.38314370807747849534 0.04771055403546069218 --0.0027036789764029569086 -0.012421968497550240837 -0.00019400613558421780209 -5 2.825345908631354893e-07 0.35527079166215922855 +-1.6298746849997449715 0.3207423054955682029 0.04670239471945906301 +-0.0021807443711779391643 -0.012535287802970449672 -0.00020920945169970240392 +5 2.825345908631354893e-07 0.3552709189640263194 0.00046732617030490929307 -4.1527454588897487753 -2.8347492039446908763 -0.081136554176388195336 -0.0041683967523185880624 0.0065946899141205552256 -0.00012065009272080269359 -6 8.459715183006415395e-08 0.43765832419088212185 +4.173466317007961557 -2.8016935252076420326 -0.081737437087388009616 +0.0041198995131368296857 0.0066275220486694394126 -0.000119701756809504006665 +6 8.459715183006415395e-08 0.43765971211410006393 0.00038925687730393611812 -6.39471595410062843 -7.621162747287802297 -0.121992225877669294154 -0.0039680130835247464163 0.0035798698934692090544 -0.00022010758050265331019 -7 1.2920249163736673626e-08 0.46960112247450473807 +6.414531809550852337 -7.603234575912382276 -0.12309230194363039723 +0.0039583234912346160553 0.003591394820962775982 -0.00021992254044702681153 +7 1.2920249163736673626e-08 0.4696151691794380732 0.00016953449859497231466 -14.793135356927480828 13.074218343364380601 -0.14311846037737518955 --0.0026297294662822792016 0.0027702756265410048361 4.4212949669357180555e-05 -8 1.5243589003230834323e-08 0.78136567314580814177 +14.779979482167510341 13.088063528768900667 -0.14289732557134240953 +-0.0026326202792006140295 0.002767798188238951903 4.424098699891899271e-05 +8 1.5243589003230834323e-08 0.7813830605782720197 0.000164587904124493665 -29.568629894896030663 -4.5543028991960081697 -0.58771107137394917874 -0.00046181040300440859715 0.0031288137434451902125 -7.498349850432879627e-05 +29.57093474400743105 -4.53865809805519671 -0.5880859062837571205 +0.00046012900387533010914 0.0031291067120909890273 -7.4950441013985698475e-05 diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swifter.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swifter.in index 3179473c0..1dbc75e21 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swifter.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swifter.in @@ -2,35 +2,35 @@ 0 0.00029591220819207775568 0.0 0.0 0.0 0.0 0.0 0.0 -1 4.9125474498983623693e-11 0.001475124456355905224 +1 4.9125474498983623693e-11 0.0014751244935834097723 1.6306381826061645943e-05 --0.30949970210807342674 0.1619004125820537876 0.041620272188990829754 --0.018820805516945871005 -0.023743802865467341506 -0.00021385162925667799668 -2 7.243452483873646905e-10 0.006759069616556246028 +-0.37723213134178928962 0.033583006382262102496 0.037347605390151236704 +-0.008342765357522348782 -0.026815373891535949219 -0.0014259978126226569104 +2 7.243452483873646905e-10 0.006759064884572926305 4.0453784346544178454e-05 --0.5567137338251560985 -0.46074173273652380134 0.02580196630219121906 -0.012753121506668980284 -0.015678149412530151263 -0.0009510907726656827677 -3 8.9970113821660187435e-10 0.010044908171483009529 +-0.48772324783973242113 -0.53438159383885197595 0.020810210727290629623 +0.014797158412775200664 -0.013730742274988789325 -0.0010423161661001279551 +3 8.9970113821660187435e-10 0.01004492566381686821 4.25875607065040958e-05 -0.6978790186886838498 -0.73607603319120218366 3.261671020506711323e-05 -0.012205130808798069983 0.0117727888369263504476 -6.0385404652521189453e-07 -4 9.549535102761465607e-11 0.0072466797341124641736 +0.75635861236241797023 -0.674672320414933413 2.9482164814591560215e-05 +0.0111724732704936106226 0.0127745538308708106445 -6.4922715710692383536e-07 +4 9.549535102761465607e-11 0.007246661019460395855 2.265740805092889601e-05 --1.617661473167097963 0.38314370807747849534 0.04771055403546069218 --0.0027036789764029569086 -0.012421968497550240837 -0.00019400613558421780209 -5 2.825345908631354893e-07 0.35527079166215922855 +-1.6298746849997449715 0.3207423054955682029 0.04670239471945906301 +-0.0021807443711779391643 -0.012535287802970449672 -0.00020920945169970240392 +5 2.825345908631354893e-07 0.3552709189640263194 0.00046732617030490929307 -4.1527454588897487753 -2.8347492039446908763 -0.081136554176388195336 -0.0041683967523185880624 0.0065946899141205552256 -0.00012065009272080269359 -6 8.459715183006415395e-08 0.43765832419088212185 +4.173466317007961557 -2.8016935252076420326 -0.081737437087388009616 +0.0041198995131368296857 0.0066275220486694394126 -0.000119701756809504006665 +6 8.459715183006415395e-08 0.43765971211410006393 0.00038925687730393611812 -6.39471595410062843 -7.621162747287802297 -0.121992225877669294154 -0.0039680130835247464163 0.0035798698934692090544 -0.00022010758050265331019 -7 1.2920249163736673626e-08 0.46960112247450473807 +6.414531809550852337 -7.603234575912382276 -0.12309230194363039723 +0.0039583234912346160553 0.003591394820962775982 -0.00021992254044702681153 +7 1.2920249163736673626e-08 0.4696151691794380732 0.00016953449859497231466 -14.793135356927480828 13.074218343364380601 -0.14311846037737518955 --0.0026297294662822792016 0.0027702756265410048361 4.4212949669357180555e-05 -8 1.5243589003230834323e-08 0.78136567314580814177 +14.779979482167510341 13.088063528768900667 -0.14289732557134240953 +-0.0026326202792006140295 0.002767798188238951903 4.424098699891899271e-05 +8 1.5243589003230834323e-08 0.7813830605782720197 0.000164587904124493665 -29.568629894896030663 -4.5543028991960081697 -0.58771107137394917874 -0.00046181040300440859715 0.0031288137434451902125 -7.498349850432879627e-05 +29.57093474400743105 -4.53865809805519671 -0.5880859062837571205 +0.00046012900387533010914 0.0031291067120909890273 -7.4950441013985698475e-05 diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swiftest.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swiftest.in index 207dd84f6..e506d4743 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swiftest.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/pl.swiftest.in @@ -1,33 +1,33 @@ 8 -1 4.9125474498983623693e-11 0.001475124456355905224 +1 4.9125474498983623693e-11 0.0014751244935834097723 1.6306381826061645943e-05 --0.30949970210807342674 0.1619004125820537876 0.041620272188990829754 --0.018820805516945871005 -0.023743802865467341506 -0.00021385162925667799668 -2 7.243452483873646905e-10 0.006759069616556246028 +-0.37723213134178928962 0.033583006382262102496 0.037347605390151236704 +-0.008342765357522348782 -0.026815373891535949219 -0.0014259978126226569104 +2 7.243452483873646905e-10 0.006759064884572926305 4.0453784346544178454e-05 --0.5567137338251560985 -0.46074173273652380134 0.02580196630219121906 -0.012753121506668980284 -0.015678149412530151263 -0.0009510907726656827677 -3 8.9970113821660187435e-10 0.010044908171483009529 +-0.48772324783973242113 -0.53438159383885197595 0.020810210727290629623 +0.014797158412775200664 -0.013730742274988789325 -0.0010423161661001279551 +3 8.9970113821660187435e-10 0.01004492566381686821 4.25875607065040958e-05 -0.6978790186886838498 -0.73607603319120218366 3.261671020506711323e-05 -0.012205130808798069983 0.0117727888369263504476 -6.0385404652521189453e-07 -4 9.549535102761465607e-11 0.0072466797341124641736 +0.75635861236241797023 -0.674672320414933413 2.9482164814591560215e-05 +0.0111724732704936106226 0.0127745538308708106445 -6.4922715710692383536e-07 +4 9.549535102761465607e-11 0.007246661019460395855 2.265740805092889601e-05 --1.617661473167097963 0.38314370807747849534 0.04771055403546069218 --0.0027036789764029569086 -0.012421968497550240837 -0.00019400613558421780209 -5 2.825345908631354893e-07 0.35527079166215922855 +-1.6298746849997449715 0.3207423054955682029 0.04670239471945906301 +-0.0021807443711779391643 -0.012535287802970449672 -0.00020920945169970240392 +5 2.825345908631354893e-07 0.3552709189640263194 0.00046732617030490929307 -4.1527454588897487753 -2.8347492039446908763 -0.081136554176388195336 -0.0041683967523185880624 0.0065946899141205552256 -0.00012065009272080269359 -6 8.459715183006415395e-08 0.43765832419088212185 +4.173466317007961557 -2.8016935252076420326 -0.081737437087388009616 +0.0041198995131368296857 0.0066275220486694394126 -0.000119701756809504006665 +6 8.459715183006415395e-08 0.43765971211410006393 0.00038925687730393611812 -6.39471595410062843 -7.621162747287802297 -0.121992225877669294154 -0.0039680130835247464163 0.0035798698934692090544 -0.00022010758050265331019 -7 1.2920249163736673626e-08 0.46960112247450473807 +6.414531809550852337 -7.603234575912382276 -0.12309230194363039723 +0.0039583234912346160553 0.003591394820962775982 -0.00021992254044702681153 +7 1.2920249163736673626e-08 0.4696151691794380732 0.00016953449859497231466 -14.793135356927480828 13.074218343364380601 -0.14311846037737518955 --0.0026297294662822792016 0.0027702756265410048361 4.4212949669357180555e-05 -8 1.5243589003230834323e-08 0.78136567314580814177 +14.779979482167510341 13.088063528768900667 -0.14289732557134240953 +-0.0026326202792006140295 0.002767798188238951903 4.424098699891899271e-05 +8 1.5243589003230834323e-08 0.7813830605782720197 0.000164587904124493665 -29.568629894896030663 -4.5543028991960081697 -0.58771107137394917874 -0.00046181040300440859715 0.0031288137434451902125 -7.498349850432879627e-05 +29.57093474400743105 -4.53865809805519671 -0.5880859062837571205 +0.00046012900387533010914 0.0031291067120909890273 -7.4950441013985698475e-05 diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb index 86a6d8098..720db909b 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb @@ -21,9 +21,9 @@ "output_type": "stream", "text": [ "Reading Swifter file param.swifter.in\n", - "Reading in time 3.650e+03\n", + "Reading in time 9.500e+03\n", "Creating Dataset\n", - "Successfully converted 366 output frames.\n", + "Successfully converted 96 output frames.\n", "Swifter simulation data stored as xarray DataSet .ds\n" ] } @@ -45,9 +45,9 @@ "output_type": "stream", "text": [ "Reading Swiftest file param.swiftest.in\n", - "Reading in time 3.650e+03\n", + "Reading in time 9.500e+03\n", "Creating Dataset\n", - "Successfully converted 366 output frames.\n", + "Successfully converted 96 output frames.\n", "Swiftest simulation data stored as xarray DataSet .ds\n" ] } @@ -104,7 +104,7 @@ "outputs": [ { "data": { - "image/png": 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\n", + "image/png": 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\n", 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" ] @@ -130,7 +130,7 @@ "outputs": [ { "data": { - "image/png": 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\n", 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\n", 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\n", 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\n", 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\n", 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\n", "text/plain": [ "
" ] @@ -230,7 +230,7 @@ }, { "cell_type": "code", - "execution_count": 28, + "execution_count": 21, "metadata": {}, "outputs": [ { @@ -587,27 +587,73 @@ " stroke: currentColor;\n", " fill: currentColor;\n", "}\n", - "
<xarray.DataArray 'px' ()>\n",
-       "array(-9.71445147e-15)\n",
+       "
<xarray.Dataset>\n",
+       "Dimensions:  (id: 16)\n",
        "Coordinates:\n",
-       "    id       int64 101\n",
-       "    time     float64 1.14e+03
"
+       "  * id       (id) int64 101 102 103 104 105 106 107 ... 111 112 113 114 115 116\n",
+       "    time     float64 500.0\n",
+       "Data variables:\n",
+       "    Gmass    (id) float64 nan nan nan nan nan nan ... nan nan nan nan nan nan\n",
+       "    Radius   (id) float64 nan nan nan nan nan nan ... nan nan nan nan nan nan\n",
+       "    px       (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 0.0 0.0\n",
+       "    py       (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 0.0 0.0\n",
+       "    pz       (id) float64 0.0 0.0 0.0 0.0 -1.775e-18 ... 0.0 -1.388e-17 0.0 0.0\n",
+       "    vx       (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 -3.469e-18\n",
+       "    vy       (id) float64 0.0 0.0 0.0 0.0 ... -4.337e-19 2.168e-19 0.0\n",
+       "    vz       (id) float64 0.0 0.0 -1.084e-19 ... -4.066e-20 -1.355e-20\n",
+       "    rmag     (id) float64 0.0 0.0 0.0 0.0 1.775e-18 ... 0.0 1.388e-17 0.0 0.0\n",
+       "    vmag     (id) float64 0.0 0.0 1.084e-19 0.0 ... 4.4e-19 2.206e-19 3.469e-18
" ], "text/plain": [ - "\n", - "array(-9.71445147e-15)\n", + "\n", + "Dimensions: (id: 16)\n", "Coordinates:\n", - " id int64 101\n", - " time float64 1.14e+03" + " * id (id) int64 101 102 103 104 105 106 107 ... 111 112 113 114 115 116\n", + " time float64 500.0\n", + "Data variables:\n", + " Gmass (id) float64 nan nan nan nan nan nan ... nan nan nan nan nan nan\n", + " Radius (id) float64 nan nan nan nan nan nan ... nan nan nan nan nan nan\n", + " px (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 0.0 0.0\n", + " py (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 0.0 0.0\n", + " pz (id) float64 0.0 0.0 0.0 0.0 -1.775e-18 ... 0.0 -1.388e-17 0.0 0.0\n", + " vx (id) float64 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 -3.469e-18\n", + " vy (id) float64 0.0 0.0 0.0 0.0 ... -4.337e-19 2.168e-19 0.0\n", + " vz (id) float64 0.0 0.0 -1.084e-19 ... -4.066e-20 -1.355e-20\n", + " rmag (id) float64 0.0 0.0 0.0 0.0 1.775e-18 ... 0.0 1.388e-17 0.0 0.0\n", + " vmag (id) float64 0.0 0.0 1.084e-19 0.0 ... 4.4e-19 2.206e-19 3.469e-18" ] }, - "execution_count": 28, + "execution_count": 21, "metadata": {}, "output_type": "execute_result" } ], "source": [ - "swiftdiff['px'].sel(id=101).isel(time=114)" + "swiftdiff.sel(id=tpidx).isel(time=5)" ] }, { diff --git a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/tp.in b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/tp.in index c1e239467..e8eeff31e 100644 --- a/examples/rmvs_swifter_comparison/8pl_16tp_encounters/tp.in +++ b/examples/rmvs_swifter_comparison/8pl_16tp_encounters/tp.in @@ -1,49 +1,49 @@ 16 101 --0.30947664140174180325 0.16192347328838543885 0.041620272188990829754 --0.01621725604493672035 -0.023743802865467341506 -0.00021385162925667799668 +-0.37720907063545766613 0.033606067088593753744 0.037347605390151236704 +-0.0057392158855131963913 -0.026815373891535949219 -0.0014259978126226569104 102 --0.30952276281440505024 0.16187735187572213635 0.041620272188990829754 --0.021424354988955021661 -0.023743802865467341506 -0.00021385162925667799668 +-0.37725519204812091312 0.033559945675930451248 0.037347605390151236704 +-0.010946314829531501173 -0.026815373891535949219 -0.0014259978126226569104 103 --0.55665652353468386693 -0.46068452244605162527 0.02580196630219121906 -0.019100355212014374223 -0.015678149412530151263 -0.0009510907726656827677 +-0.48766603754926024505 -0.53432438354837974437 0.020810210727290629623 +0.021144392118120594604 -0.013730742274988789325 -0.0010423161661001279551 104 --0.5567709441156283301 -0.4607989430269959774 0.02580196630219121906 -0.0064058878013235863447 -0.015678149412530151263 -0.0009510907726656827677 +-0.4877804581302045972 -0.53443880412932420754 0.020810210727290629623 +0.008449924707429806725 -0.013730742274988789325 -0.0010423161661001279551 105 -0.6979392465946233637 -0.7360158052852626698 3.261671020506711323e-05 -0.019099571043071944532 0.0117727888369263504476 -6.0385404652521189453e-07 +0.7564188402683574841 -0.6746120925089938991 2.9482164814591560215e-05 +0.018066913504767485171 0.0127745538308708106445 -6.4922715710692383536e-07 106 -0.6978187907827443359 -0.73613626109714169754 3.261671020506711323e-05 -0.005310690574524194567 0.0117727888369263504476 -6.0385404652521189453e-07 +0.75629838445647845635 -0.67473254832087292687 2.9482164814591560215e-05 +0.0042780330362197352065 0.0127745538308708106445 -6.4922715710692383536e-07 107 --1.6176294307533440886 0.38317575049123231423 0.04771055403546069218 -0.00037580012182093606998 -0.012421968497550240837 -0.00019400613558421780209 +-1.6298426425859910971 0.3207743479093220218 0.04670239471945906301 +0.00089873472704595381427 -0.012535287802970449672 -0.00020920945169970240392 108 --1.6176935155808518374 0.38311166566372467646 0.04771055403546069218 --0.005783158074626849887 -0.012421968497550240837 -0.00019400613558421780209 +-1.6299067274134988459 0.32071026308181438402 0.04670239471945906301 +-0.005260223469401832143 -0.012535287802970449672 -0.00020920945169970240392 109 -4.1534063578978459574 -2.834088304936593694 -0.081136554176388195336 -0.041050613953966016978 0.0065946899141205552256 -0.00012065009272080269359 +4.174127216016058739 -2.8010326261995448505 -0.081737437087388009616 +0.041002116714784257734 0.0066275220486694394126 -0.000119701756809504006665 110 -4.152084559881651593 -2.8354101029527880584 -0.081136554176388195336 --0.032713820449328842588 0.0065946899141205552256 -0.00012065009272080269359 +4.1728054179998643747 -2.8023544242157392148 -0.081737437087388009616 +-0.032762317688510601832 0.0066275220486694394126 -0.000119701756809504006665 111 -6.395266446455758924 -7.620612254932671803 -0.121992225877669294154 -0.026081181967058334609 0.0035798698934692090544 -0.00022010758050265331019 +6.415082301905982831 -7.602684083557251782 -0.12309230194363039723 +0.026071492374768204248 0.003591394820962775982 -0.00021992254044702681153 112 -6.394165461745497936 -7.621713239642932791 -0.121992225877669294154 --0.01814515580000884351 0.0035798698934692090544 -0.00022010758050265331019 +6.413981317195721843 -7.60378506826751277 -0.12309230194363039723 +-0.018154845392298973872 0.003591394820962775982 -0.00021992254044702681153 113 -14.793375114914683266 13.074458101351583039 -0.14311846037737518955 -0.0104650340723796142495 0.0027702756265410048361 4.4212949669357180555e-05 +14.780219240154712779 13.088303286756103105 -0.14289732557134240953 +0.010462143259461278988 0.002767798188238951903 4.424098699891899271e-05 114 -14.79289559894027839 13.073978585377178163 -0.14311846037737518955 --0.015724493004944172653 0.0027702756265410048361 4.4212949669357180555e-05 +14.779739724180307903 13.087823770781698229 -0.14289732557134240953 +-0.015727383817862507914 0.002767798188238951903 4.424098699891899271e-05 115 -29.568862657342247502 -4.5540701367497931074 -0.58771107137394917874 -0.0148974462162825404404 0.0031288137434451902125 -7.498349850432879627e-05 +29.571167506453647889 -4.538425335608981648 -0.5880859062837571205 +0.01489576481715346179 0.0031291067120909890273 -7.4950441013985698475e-05 116 -29.568397132449813824 -4.554535661642223232 -0.58771107137394917874 --0.013973825410273721728 0.0031288137434451902125 -7.498349850432879627e-05 +29.570701981561214211 -4.5388908605014117725 -0.5880859062837571205 +-0.013975506809402800379 0.0031291067120909890273 -7.4950441013985698475e-05 diff --git a/examples/rmvs_swifter_comparison/mars_ejecta/pl.swifter.in b/examples/rmvs_swifter_comparison/mars_ejecta/pl.swifter.in index ab7f6ec08..bef7f7500 100644 --- a/examples/rmvs_swifter_comparison/mars_ejecta/pl.swifter.in +++ b/examples/rmvs_swifter_comparison/mars_ejecta/pl.swifter.in @@ -2,7 +2,7 @@ 1 2.9591220828563E-04 .0 .0 .0 .0 .0 .0 - 2 4.912576812862670E-11 1.475E-03 ! Mercury / Mass (Msun) / Rhill (AU) + 2 4.912576812862670E-11 1.475E-03 ! Mercury / Mass (Msun) / rhill (AU) 1.63104E-05 ! Radius (AU) 3.347381871776144E-01 -2.106110537919978E-01 -4.792146121659843E-02 9.457239437449661E-03 2.510612575783642E-02 1.183593414707043E-03 diff --git a/examples/symba_chambers_2013/.gitignore b/examples/symba_chambers_2013/.gitignore new file mode 100644 index 000000000..18e3d4488 --- /dev/null +++ b/examples/symba_chambers_2013/.gitignore @@ -0,0 +1 @@ +savestate/* diff --git a/examples/symba_chambers_2013/.idea/.gitignore b/examples/symba_chambers_2013/.idea/.gitignore new file mode 100644 index 000000000..26d33521a --- /dev/null +++ b/examples/symba_chambers_2013/.idea/.gitignore @@ -0,0 +1,3 @@ +# Default ignored files +/shelf/ +/workspace.xml diff --git a/examples/symba_chambers_2013/aescattermovie.py b/examples/symba_chambers_2013/aescattermovie.py new file mode 100755 index 000000000..6f73a32dc --- /dev/null +++ b/examples/symba_chambers_2013/aescattermovie.py @@ -0,0 +1,124 @@ +#!/usr/bin/env python3 +import swiftest +import numpy as np +import matplotlib.pyplot as plt +from matplotlib import animation +import matplotlib.colors as mcolors + +titletext = "Chambers (2013)" +radscale = 2000 +AU = 1.0 +xmin = 0.0 +xmax = 2.00 +ymin = 1e-4 +ymax = 1.0 +framejump = 1 +ncutoff = 1e20 + +class AnimatedScatter(object): + """An animated scatter plot using matplotlib.animations.FuncAnimation.""" + def __init__(self, ds, param): + + frame = 0 + nframes = int(ds['time'].size / framejump) + self.ds = ds + self.param = param + self.Rcb = self.ds['radius'].sel(id=0, time=0).values + + self.clist = {'Initial conditions' : 'xkcd:faded blue', + 'Disruption' : 'xkcd:marigold', + 'Supercatastrophic' : 'xkcd:shocking pink', + 'Hit and run fragment' : 'xkcd:baby poop green'} + + # Setup the figure and axes... + fig = plt.figure(figsize=(8,4.5), dpi=300) + plt.tight_layout(pad=0) + # set up the figure + self.ax = plt.Axes(fig, [0.1, 0.15, 0.8, 0.75]) + self.ax.set_xlim(xmin, xmax) + self.ax.set_ylim(ymin, ymax) + fig.add_axes(self.ax) + self.ani = animation.FuncAnimation(fig, self.update, interval=1, frames=nframes, init_func=self.setup_plot, blit=True) + #self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'libx264']) + self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'mpeg4']) + print('Finished writing aescattter.mp4') + + def scatters(self, pl, radmarker, origin): + scat = [] + for key, value in self.clist.items(): + idx = origin == key + s = self.ax.scatter(pl[idx, 0], pl[idx, 1], marker='o', s=radmarker[idx], c=value, alpha=0.75, label=key) + scat.append(s) + return scat + + def setup_plot(self): + # First frame + """Initial drawing of the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(0)) + + # set up the figure + self.ax.margins(x=10, y=1) + self.ax.set_xlabel("Semi Major Axis (AU)", fontsize='16', labelpad=1) + self.ax.set_ylabel("Eccentricity", fontsize='16', labelpad=1) + self.ax.set_yscale("log") + + self.title = self.ax.text(0.50, 1.05, "", bbox={'facecolor': 'w', 'alpha': 0.5, 'pad': 5}, transform=self.ax.transAxes, + ha="center") + + self.title.set_text(f"{titletext} - Time = ${t*1e-6:6.3f}$ My with ${npl:4.0f}$ particles") + slist = self.scatters(pl, radmarker, origin) + self.s0 = slist[0] + self.s1 = slist[1] + self.s2 = slist[2] + self.s3 = slist[3] + leg = plt.legend(loc="lower right", scatterpoints=1, fontsize=10) + for i,l in enumerate(leg.legendHandles): + leg.legendHandles[i]._sizes = [20] + return self.s0, self.s1, self.s2, self.s3, self.title + + def data_stream(self, frame=0): + while True: + d = self.ds.isel(time = frame) + d = d.where(d['radius'] < self.Rcb, drop=True) + d['radmarker'] = (d['radius'] / self.Rcb) * radscale + radius = d['radmarker'].values + + radius = d['radmarker'].values + Gmass = d['Gmass'].values + a = d['a'].values / AU + e = d['e'].values + name = d['id'].values + npl = d['npl'].values[0] + radmarker = d['radmarker'] + origin = d['origin_type'] + + t = self.ds.coords['time'].values[frame] + + yield t, name, Gmass, radius, npl, np.c_[a, e], radmarker, origin + + def update(self,frame): + """Update the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(framejump * frame)) + + self.title.set_text(f"{titletext} - Time = ${t*1e-6:6.3f}$ My with ${npl:4.0f}$ particles") + + # We need to return the updated artist for FuncAnimation to draw.. + # Note that it expects a sequence of artists, thus the trailing comma. + s = [self.s0, self.s1, self.s2, self.s3] + for i, (key, value) in enumerate(self.clist.items()): + idx = origin == key + s[i].set_sizes(radmarker[idx]) + s[i].set_offsets(pl[idx,:]) + s[i].set_facecolor(value) + + self.s0 = s[0] + self.s1 = s[1] + self.s2 = s[2] + self.s3 = s[3] + return self.s0, self.s1, self.s2, self.s3, self.title, + +sim = swiftest.Simulation(param_file="param.in") +sim.bin2xr() +print('Making animation') +anim = AnimatedScatter(sim.ds,sim.param) +print('Animation finished') diff --git a/examples/symba_chambers_2013/init_cond.py b/examples/symba_chambers_2013/init_cond.py new file mode 100755 index 000000000..a3225caf4 --- /dev/null +++ b/examples/symba_chambers_2013/init_cond.py @@ -0,0 +1,102 @@ +#!/usr/bin/env python3 +import swiftest +import numpy as np +from numpy.random import default_rng + +# Initialize simulation object +sim = swiftest.Simulation() + +# Set unit conversion factors +MU2KG = swiftest.MSun +TU2S = swiftest.YR2S +DU2M = swiftest.AU2M +GU = swiftest.GC / (DU2M**3 / (MU2KG * TU2S**2)) +sim.param['MU2KG'] = MU2KG +sim.param['TU2S'] = TU2S +sim.param['DU2M'] = DU2M + +# Simulation time parameters +sim.param['T0'] = 0.0 +sim.param['TSTOP'] = 300e6 +sim.param['DT'] = 6 * swiftest.JD2S / sim.param['TU2S'] +t_print = 1000.0 +iout = int(np.ceil(t_print / sim.param['DT'])) +sim.param['ISTEP_OUT'] = iout +sim.param['ISTEP_DUMP'] = iout + +# Optional output file names +sim.param['PARTICLE_OUT'] = "particle.dat" +sim.param['ENERGY'] = "YES" +sim.param['ENERGY_OUT'] = "energy.dat" +sim.param['PL_IN'] = "pl_chambers_2013.in" +sim.param['CB_IN'] = "sun_MsunAUYR.in" +sim.param['ENC_OUT'] = "" + +# Simulation parameters +sim.param['FRAGMENTATION'] = "YES" +sim.param['ROTATION'] = "YES" +sim.param['CHK_RMAX'] = 1000.0 +sim.param['CHK_EJECT'] = 1000.0 +sim.param['IN_FORM'] = 'EL' +sim.param['OUT_FORM'] = 'XVEL' +sim.param['OUT_TYPE'] = 'NETCDF_DOUBLE' +sim.param['BIN_OUT'] = 'bin.nc' + +# Add central body +sim.add("Sun") +GMcb = sim.ds['Gmass'].values[0] +sim.add("Jupiter") +sim.add("Saturn") + +# Add bodies described in Chambers (2013) Sec. 2.1, with the uniform spatial distribution and two bodies sizes (big and small) +Nb = 14 +Ns = 140 +Mb = 2.8e-7 +Ms = 2.8e-8 +dens = 3000.0 / (MU2KG / DU2M**3) +Rb = (3 * Mb / (4 * np.pi * dens) )**(1.0 / 3.0) +Rs = (3 * Ms / (4 * np.pi * dens) )**(1.0 / 3.0) +sim.param['GMTINY'] = 1e-2 * GU * Ms +sim.param['MIN_GMFRAG'] = 1e-4 * GU * Ms + +# Define the initial orbital elements of the big and small bodies +avalb = default_rng().uniform(0.3, 2.0, Nb) +avals = default_rng().uniform(0.3, 2.0, Ns) +evalb = default_rng().uniform(0.0, 0.01, Nb) +evals = default_rng().uniform(0.0, 0.01, Ns) +incvalb = default_rng().uniform(0.0, 0.5, Nb) +incvals = default_rng().uniform(0.0, 0.5, Ns) +capomvalb = default_rng().uniform(0.0, 360.0, Nb) +capomvals = default_rng().uniform(0.0, 360.0, Ns) +omegavalb = default_rng().uniform(0.0, 360.0, Nb) +omegavals = default_rng().uniform(0.0, 360.0, Ns) +capmvalb = default_rng().uniform(0.0, 360.0, Nb) +capmvals = default_rng().uniform(0.0, 360.0, Ns) +GMvalb = np.full(Nb, Mb * GU) +GMvals = np.full(Ns, Ms * GU) +Rvalb = np.full(Nb, Rb) +Rvals = np.full(Ns, Rs) +Rhb = avalb * (GMvalb / (3 * GMcb))**(1.0/3.0) +Rhs = avals * (GMvals / (3 * GMcb))**(1.0/3.0) + +# Give the bodies unique ids +idb = np.arange(10, 10 + Nb) +ids = np.arange(11 + Nb, 11 + Nb + Ns) + +nameb = [] +for i in idb: + nameb.append(f"BigBody{i-9:0.4g}") +names = [] +for i in ids: + names.append(f"SmallBody{i-9:0.4g}") + + +# Populate the simulation object with the two types of bodies +sim.addp(idb, nameb, avalb, evalb, incvalb, capomvalb, omegavalb, capmvalb, GMpl=GMvalb, Rpl=Rvalb, rhill=Rhb) +sim.addp(ids, names, avals, evals, incvals, capomvals, omegavals, capmvals, GMpl=GMvals, Rpl=Rvals, rhill=Rhs) + +# Save everything to a set of initial conditions files +sim.save("param.in") + + + diff --git a/examples/symba_chambers_2013/param.in b/examples/symba_chambers_2013/param.in new file mode 100644 index 000000000..8f200df67 --- /dev/null +++ b/examples/symba_chambers_2013/param.in @@ -0,0 +1,38 @@ +! VERSION Swiftest parameter input +T0 0.0 +TSTOP 300000000.0 +DT 0.01642710472279261 +ISTEP_OUT 60876 +ISTEP_DUMP 60876 +OUT_FORM XVEL +OUT_TYPE NETCDF_DOUBLE +OUT_STAT REPLACE +IN_TYPE ASCII +PL_IN pl_chambers_2013.in +TP_IN tp.in +CB_IN sun_MsunAUYR.in +BIN_OUT bin.nc +CHK_QMIN -1.0 +CHK_RMIN -1.0 +CHK_RMAX 1000.0 +CHK_EJECT 1000.0 +CHK_QMIN_COORD HELIO +CHK_QMIN_RANGE -1.0 -1.0 +MU2KG 1.988409870698051e+30 +TU2S 31557600.0 +DU2M 149597870700.0 +IN_FORM EL +EXTRA_FORCE NO +DISCARD_OUT discard.out +PARTICLE_OUT particle.dat +BIG_DISCARD NO +CHK_CLOSE YES +RHILL_PRESENT YES +FRAGMENTATION YES +ROTATION YES +TIDES NO +ENERGY YES +GR NO +ENERGY_OUT energy.dat +GMTINY 1.1053539394491336e-08 +MIN_GMFRAG 1.1053539394491336e-10 diff --git a/examples/symba_chambers_2013/pl_chambers_2013.in b/examples/symba_chambers_2013/pl_chambers_2013.in new file mode 100644 index 000000000..d694bd90c --- /dev/null +++ b/examples/symba_chambers_2013/pl_chambers_2013.in @@ -0,0 +1,937 @@ +156 +Jupiter 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100644 index 000000000..573541ac9 --- /dev/null +++ b/examples/symba_chambers_2013/tp.in @@ -0,0 +1 @@ +0 diff --git a/examples/symba_clement_2018/ConvertRhill.ipynb b/examples/symba_clement_2018/ConvertRhill.ipynb new file mode 100644 index 000000000..d610b4e7d --- /dev/null +++ b/examples/symba_clement_2018/ConvertRhill.ipynb @@ -0,0 +1,543 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": 1, + "metadata": {}, + "outputs": [], + "source": [ + "import swiftest" + ] + }, + { + "cell_type": "code", + "execution_count": 2, + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Reading Swiftest file param.in\n" + ] + } + ], + "source": [ + "sim = sim = swiftest.Simulation(param_file=\"param.in\")" + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Reading in time 9.900e+03\n", + "Creating Dataset\n", + "Successfully converted 100 output frames.\n", + "\n", + "Adding particle info to Dataset\n", + "Swiftest simulation data stored as xarray DataSet .ds\n" + ] + } + ], + "source": [ + "sim.bin2xr()" + ] + }, + { + "cell_type": "code", + "execution_count": 5, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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(2018)" +radscale = 2000 +AU = 1.0 +xmin = 0.0 +xmax = 2.00 +ymin = 1e-4 +ymax = 1.0 +framejump = 1 +ncutoff = 1e20 + +class AnimatedScatter(object): + """An animated scatter plot using matplotlib.animations.FuncAnimation.""" + def __init__(self, ds, param): + + frame = 0 + nframes = int(ds['time'].size / framejump) + self.ds = ds + self.param = param + self.Rcb = self.ds['radius'].sel(id=0, time=0).values + + self.clist = {'Initial conditions' : 'xkcd:faded blue', + 'Disruption' : 'xkcd:marigold', + 'Supercatastrophic' : 'xkcd:shocking pink', + 'Hit and run fragment' : 'xkcd:baby poop green'} + + # Setup the figure and axes... + fig = plt.figure(figsize=(8,4.5), dpi=300) + plt.tight_layout(pad=0) + # set up the figure + self.ax = plt.Axes(fig, [0.1, 0.15, 0.8, 0.75]) + self.ax.set_xlim(xmin, xmax) + self.ax.set_ylim(ymin, ymax) + fig.add_axes(self.ax) + self.ani = animation.FuncAnimation(fig, self.update, interval=1, frames=nframes, init_func=self.setup_plot, blit=True) + #self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'libx264']) + self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'mpeg4']) + print('Finished writing aescattter.mp4') + + def scatters(self, pl, radmarker, origin): + scat = [] + for key, value in self.clist.items(): + idx = origin == key + s = self.ax.scatter(pl[idx, 0], pl[idx, 1], marker='o', s=radmarker[idx], c=value, alpha=0.75, label=key) + scat.append(s) + return scat + + def setup_plot(self): + # First frame + """Initial drawing of the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(0)) + + # set up the figure + self.ax.margins(x=10, y=1) + self.ax.set_xlabel("Semi Major Axis (AU)", fontsize='16', labelpad=1) + self.ax.set_ylabel("Eccentricity", fontsize='16', labelpad=1) + self.ax.set_yscale("log") + + self.title = self.ax.text(0.50, 1.05, "", bbox={'facecolor': 'w', 'alpha': 0.5, 'pad': 5}, transform=self.ax.transAxes, + ha="center") + + self.title.set_text(f"{titletext} - Time = ${t*1e-6:6.3f}$ My with ${npl:4.0f}$ particles") + slist = self.scatters(pl, radmarker, origin) + self.s0 = slist[0] + self.s1 = slist[1] + self.s2 = slist[2] + self.s3 = slist[3] + leg = plt.legend(loc="lower right", scatterpoints=1, fontsize=10) + for i,l in enumerate(leg.legendHandles): + leg.legendHandles[i]._sizes = [20] + return self.s0, self.s1, self.s2, self.s3, self.title + + def data_stream(self, frame=0): + while True: + d = self.ds.isel(time = frame) + d = d.where(d['radius'] < self.Rcb, drop=True) + d['radmarker'] = (d['radius'] / self.Rcb) * radscale + radius = d['radmarker'].values + + radius = d['radmarker'].values + Gmass = d['Gmass'].values + a = d['a'].values / AU + e = d['e'].values + name = d['id'].values + npl = d['npl'].values[0] + radmarker = d['radmarker'] + origin = d['origin_type'] + + t = self.ds.coords['time'].values[frame] + + yield t, name, Gmass, radius, npl, np.c_[a, e], radmarker, origin + + def update(self,frame): + """Update the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(framejump * frame)) + + self.title.set_text(f"{titletext} - Time = ${t*1e-6:6.3f}$ My with ${npl:4.0f}$ particles") + + # We need to return the updated artist for FuncAnimation to draw.. + # Note that it expects a sequence of artists, thus the trailing comma. + s = [self.s0, self.s1, self.s2, self.s3] + for i, (key, value) in enumerate(self.clist.items()): + idx = origin == key + s[i].set_sizes(radmarker[idx]) + s[i].set_offsets(pl[idx,:]) + s[i].set_facecolor(value) + + self.s0 = s[0] + self.s1 = s[1] + self.s2 = s[2] + self.s3 = s[3] + return self.s0, self.s1, self.s2, self.s3, self.title, + +sim = swiftest.Simulation(param_file="param.in") +sim.bin2xr() +print('Making animation') +anim = AnimatedScatter(sim.ds,sim.param) +print('Animation finished') diff --git a/examples/symba_clement_2018/param.in b/examples/symba_clement_2018/param.in new file mode 100644 index 000000000..6f58b1822 --- /dev/null +++ b/examples/symba_clement_2018/param.in @@ -0,0 +1,37 @@ +! 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" + ], + "text/plain": [ + "\n", + "Dimensions: (id: 3, time: 301)\n", + "Coordinates:\n", + " * time (time) float64 0.0 1e-07 2e-07 ... 2.98e-05 2.99e-05 3e-05\n", + " * id (id) int32 0 1 2\n", + "Data variables: (12/57)\n", + " npl (time, id) float64 2.0 2.0 2.0 2.0 ... 20.0 20.0 20.0 20.0\n", + " ntp (time, id) float64 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0\n", + " name (id) object b'0' b'1' b'2'\n", + " particle_type (id) object b'Central Body' b'Massive Body' b'Massive Body'\n", + " xhx (time, id) float64 0.0 1.0 1.0 0.0 1.0 ... 0.0 0.0 0.0 0.0\n", + " xhy (time, id) float64 0.0 -4.2e-05 4.2e-05 0.0 ... 0.0 0.0 0.0\n", + " ... ...\n", + " discard_xhy (id) float64 -2.736e+299 -5.125e-06 5.125e-06\n", + " discard_xhz (id) float64 0.0 0.0 0.0\n", + " discard_vhx (id) float64 2.171e-314 -0.0002318 -0.0002318\n", + " discard_vhy (id) float64 0.0 6.28 -6.281\n", + " discard_vhz (id) float64 2.171e-314 0.0 0.0\n", + " discard_body_id (id) float64 -2.147e+09 -2.147e+09 -2.147e+09" + ] + }, + "execution_count": 11, + "metadata": {}, + "output_type": "execute_result" + } + ], + "source": [ + "ds1" + ] + }, + { + "cell_type": "code", + "execution_count": null, + "metadata": {}, + "outputs": [], + "source": [] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.8.6" + } + }, + "nbformat": 4, + "nbformat_minor": 4 +} diff --git a/examples/symba_energy_momentum/collision_movie.py b/examples/symba_energy_momentum/collision_movie.py index 3fd3b6a86..4f472d9ff 100755 --- a/examples/symba_energy_momentum/collision_movie.py +++ b/examples/symba_energy_momentum/collision_movie.py @@ -10,44 +10,50 @@ xmax = 20.0 ymin = -20.0 ymax = 20.0 - -cases = ['supercat_head', 'supercat_off', 'disruption_head', 'disruption_off'] - -def scale_sim(ds): - +framejump = 1 +ncutoff = 1e20 +radscale = 2000 + +#cases = ['supercat_head', 'supercat_off', 'disruption_head', 'disruption_off'] +cases = ['disruption_off'] + +def scale_sim(ds, Rcb): + dst0 = ds.isel(time=0) + dst0 = dst0.where(dst0['radius'] < Rcb, drop=True) + dst0 = dst0.where(dst0.id > 0, drop=True) + GMtot = dst0['Gmass'].sum(skipna=True, dim="id") dsscale = ds.where(ds.id > 0, drop=True) # Remove the central body + + rscale = ds['radius'].sel(id=1, time=0).values + dsscale['radius'] /= rscale - GMtot = dsscale['GMass'].sum(skipna=True, dim="id").isel(time=0) - rscale = ds['Radius'].sel(id=1, time=0) - dsscale['Radius'] /= rscale + dsscale['radmarker'] = dsscale['radius'].fillna(0) - dsscale['radmarker'] = dsscale['Radius'].fillna(0) + dsscale['xhx'] /= rscale + dsscale['xhy'] /= rscale + dsscale['xhz'] /= rscale - dsscale['px'] /= rscale - dsscale['py'] /= rscale - dsscale['pz'] /= rscale - - mpx = dsscale['GMass'] * dsscale['px'] - mpy = dsscale['GMass'] * dsscale['py'] - mpz = dsscale['GMass'] * dsscale['pz'] - xbsys = mpx.sum(skipna=True, dim="id") / GMtot + mxhx = dsscale['Gmass'] * dsscale['xhx'] + mpy = dsscale['Gmass'] * dsscale['xhy'] + mpz = dsscale['Gmass'] * dsscale['xhz'] + xbsys = mxhx.sum(skipna=True, dim="id") / GMtot ybsys = mpy.sum(skipna=True, dim="id") / GMtot zbsys = mpz.sum(skipna=True, dim="id") / GMtot - mvx = dsscale['GMass'] * dsscale['vx'] - mvy = dsscale['GMass'] * dsscale['vy'] - mvz = dsscale['GMass'] * dsscale['vz'] - vxbsys = mvx.sum(skipna=True, dim="id") / GMtot - vybsys = mvy.sum(skipna=True, dim="id") / GMtot - vzbsys = mvz.sum(skipna=True, dim="id") / GMtot + mvx = dsscale['Gmass'] * dsscale['vhx'] + mvy = dsscale['Gmass'] * dsscale['vhy'] + mvz = dsscale['Gmass'] * dsscale['vhz'] + vhxbsys = mvx.sum(skipna=True, dim="id") / GMtot + vhybsys = mvy.sum(skipna=True, dim="id") / GMtot + vhzbsys = mvz.sum(skipna=True, dim="id") / GMtot - dsscale['pxb'] = dsscale['px'] - xbsys - dsscale['pyb'] = dsscale['py'] - ybsys - dsscale['pzb'] = dsscale['pz'] - zbsys + dsscale['xhxb'] = dsscale['xhx'] - xbsys + dsscale['pyb'] = dsscale['xhy'] - ybsys + dsscale['pzb'] = dsscale['xhz'] - zbsys - dsscale['vxb'] = dsscale['vx'] - vxbsys - dsscale['vyb'] = dsscale['vy'] - vybsys - dsscale['vzb'] = dsscale['vz'] - vzbsys + dsscale['vhxb'] = dsscale['vhx'] - vhxbsys + dsscale['vhyb'] = dsscale['vhy'] - vhybsys + dsscale['vhzb'] = dsscale['vhz'] - vhzbsys return dsscale @@ -64,12 +70,12 @@ class AnimatedScatter(object): """An animated scatter plot using matplotlib.animations.FuncAnimation.""" def __init__(self, ds, param): - frame = 0 - nframes = ds['time'].size - self.ds = scale_sim(ds) + nframes = int(ds['time'].size / framejump) self.param = param + self.Rcb = ds['radius'].sel(id=0, time=0).values self.rot_angle = {} + self.ds = scale_sim(ds, self.Rcb) self.clist = {'Initial conditions' : 'xkcd:windows blue', 'Disruption' : 'xkcd:baby poop', @@ -94,8 +100,9 @@ def __init__(self, ds, param): # Then setup FuncAnimation. self.ani = animation.FuncAnimation(fig, self.update, interval=1, frames=nframes, init_func=self.setup_plot, blit=False) - self.ani.save(animfile, fps=60, dpi=300, - extra_args=['-vcodec', 'libx264']) + #self.ani.save(animfile, fps=60, dpi=300, extra_args=['-vcodec', 'mpeg4']) + self.ani.save(animfile, fps=60, dpi=300, extra_args=['-vcodec', 'libx264']) + print(f"Finished writing {animfile}") def plot_pl_circles(self, pl, radmarker): patches = [] @@ -155,27 +162,27 @@ def origin_to_color(self, origin): return cval def velocity_vectors(self, pl, r): - px = pl[:, 0] + xhx = pl[:, 0] py = pl[:, 1] - vx = pl[:, 2] - vy = pl[:, 3] - vmag = np.sqrt(vx ** 2 + vy ** 2) - ux = np.zeros_like(vx) - uy = np.zeros_like(vx) + vhx = pl[:, 2] + vhy = pl[:, 3] + vmag = np.sqrt(vhx ** 2 + vhy ** 2) + ux = np.zeros_like(vhx) + uy = np.zeros_like(vhx) goodv = vmag > 0.0 - ux[goodv] = vx[goodv] / vmag[goodv] - uy[goodv] = vy[goodv] / vmag[goodv] + ux[goodv] = vhx[goodv] / vmag[goodv] + uy[goodv] = vhy[goodv] / vmag[goodv] varrowend = [] varrowtip = [] for i in range(pl.shape[0]): - vend = (px[i], py[i]) - vtip = (px[i] + vx[i] * self.v_length, py[i] + vy[i] * self.v_length) + vend = (xhx[i], py[i]) + vtip = (xhx[i] + vhx[i] * self.v_length, py[i] + vhy[i] * self.v_length) varrowend.append(vend) varrowtip.append(vtip) return varrowend, varrowtip def spin_arrows(self, pl, id, len): - px = pl[:, 0] + xhx = pl[:, 0] py = pl[:, 1] sarrowend = [] sarrowtip = [] @@ -185,8 +192,8 @@ def spin_arrows(self, pl, id, len): r = R.from_rotvec(self.rot_angle[id[i]]) endrel = r.apply(endrel) tiprel = r.apply(tiprel) - send = (px[i] + endrel[0], py[i] + endrel[1]) - stip = (px[i] + tiprel[0], py[i] + tiprel[1]) + send = (xhx[i] + endrel[0], py[i] + endrel[1]) + stip = (xhx[i] + tiprel[0], py[i] + tiprel[1]) sarrowend.append(send) sarrowtip.append(stip) return sarrowend, sarrowtip @@ -194,7 +201,7 @@ def spin_arrows(self, pl, id, len): def setup_plot(self): # First frame """Initial drawing of the scatter plot.""" - t, name, GMass, Radius, npl, pl, radmarker, origin = next(self.data_stream(0)) + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(0)) cval = self.origin_to_color(origin) @@ -220,7 +227,7 @@ def setup_plot(self): def update(self,frame): """Update the scatter plot.""" - t, name, GMass, Radius, npl, pl, radmarker, origin = next(self.data_stream(frame)) + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(frame)) cval = self.origin_to_color(origin) varrowend, varrowtip = self.velocity_vectors(pl, radmarker) sarrowend, sarrowtip = self.spin_arrows(pl, name, radmarker) @@ -239,32 +246,33 @@ def update(self,frame): def data_stream(self, frame=0): while True: d = self.ds.isel(time=frame) - Radius = d['radmarker'].values - GMass = d['GMass'].values - x = d['pxb'].values + #d = d.where(d['radius'] > 0.0, drop=True) + radius = d['radius'].values + Gmass = d['Gmass'].values + x = d['xhxb'].values y = d['pyb'].values - vx = d['vxb'].values - vy = d['vyb'].values + vhx = d['vhxb'].values + vhy = d['vhyb'].values name = d['id'].values - npl = d.id.count().values + npl = d['npl'].values[0] id = d['id'].values - rotx = d['rot_x'].values - roty = d['rot_y'].values - rotz = d['rot_z'].values + rotx = d['rotx'].values + roty = d['roty'].values + rotz = d['rotz'].values radmarker = d['radmarker'].values origin = d['origin_type'].values t = self.ds.coords['time'].values[frame] - self.mask = np.logical_not(np.isnan(x)) + self.mask = np.logical_not(radius == 0.0) x = np.nan_to_num(x, copy=False) y = np.nan_to_num(y, copy=False) - vx = np.nan_to_num(vx, copy=False) - vy = np.nan_to_num(vy, copy=False) + vhx = np.nan_to_num(vhx, copy=False) + vhy = np.nan_to_num(vhy, copy=False) radmarker = np.nan_to_num(radmarker, copy=False) - GMass = np.nan_to_num(GMass, copy=False) - Radius = np.nan_to_num(Radius, copy=False) + Gmass = np.nan_to_num(Gmass, copy=False) + radius = np.nan_to_num(radius, copy=False) rotx = np.nan_to_num(rotx, copy=False) roty = np.nan_to_num(roty, copy=False) rotz = np.nan_to_num(rotz, copy=False) @@ -281,7 +289,7 @@ def data_stream(self, frame=0): for i in id[idxactive]: self.rot_angle[i] = self.rot_angle[i] + dt * np.array(self.rotvec[i]) frame += 1 - yield t, name, GMass, Radius, npl, np.c_[x, y, vx, vy], radmarker, origin + yield t, name, Gmass, radius, npl, np.c_[x, y, vhx, vhy], radmarker, origin for case in cases: if case == 'supercat_off': @@ -304,6 +312,10 @@ def data_stream(self, frame=0): animfile = 'movies/merger.mp4' titletext = "Merger" paramfile = 'param.merger.in' + elif case == 'hit_and_run': + animfile = 'movies/hitandrun.mp4' + titletext = "Hit and run with fragmentation" + paramfile = 'param.hitandrun.in' else: print(f'{case} is an unknown case') exit(-1) diff --git a/examples/symba_energy_momentum/hitandrun.in b/examples/symba_energy_momentum/hitandrun.in new file mode 100644 index 000000000..45f3654f8 --- /dev/null +++ b/examples/symba_energy_momentum/hitandrun.in @@ -0,0 +1,13 @@ +2 +1 1e-07 0.0009 +7e-06 +1.0 -4.20E-05 0.0 +0.00 6.28 0.0 +0.4 0.4 0.4 !Ip +0.0 0.0 6.0e4 !rot +2 7e-10 0.0004 +3.25e-06 +1.0 4.20E-05 0.0 +-1.50 -6.28 0.0 +0.4 0.4 0.4 !Ip +0.0 0.0 1.0e5 !rot diff --git a/examples/symba_energy_momentum/param.disruption_headon.in b/examples/symba_energy_momentum/param.disruption_headon.in index 4a291535e..a012c5505 100644 --- a/examples/symba_energy_momentum/param.disruption_headon.in +++ b/examples/symba_energy_momentum/param.disruption_headon.in @@ -1,15 +1,15 @@ T0 0.0e0 -TSTOP 0.000100 ! simulation length in seconds = 100 years -DT 0.0000001 ! stepsize in seconds +TSTOP 0.0001000 ! simulation length in seconds = 100 years +DT 0.0000001 ! stepsize in seconds CB_IN cb.in PL_IN disruption_headon.in TP_IN tp.in IN_TYPE ASCII ISTEP_OUT 1 ! output cadence every year -BIN_OUT bin.disruption_headon.dat +BIN_OUT bin.disruption_headon.nc PARTICLE_OUT particle.disruption_headon.dat -OUT_TYPE REAL8 ! double precision real output -OUT_FORM XV ! osculating element output +OUT_TYPE NETCDF_DOUBLE ! double precision real output +OUT_FORM XVEL ! osculating element output OUT_STAT REPLACE ISTEP_DUMP 1 ! system dump cadence CHK_CLOSE yes ! check for planetary close encounters @@ -21,7 +21,8 @@ ENC_OUT enc.disruption_headon.dat EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded RHILL_PRESENT yes ! Hill's sphere radii in input file -GMTINY 1.0e-16 +GMTINY 1.0e-11 +MIN_GMFRAG 1.0e-11 FRAGMENTATION yes MU2KG 1.98908e30 TU2S 3.1556925e7 diff --git a/examples/symba_energy_momentum/param.disruption_off_axis.in b/examples/symba_energy_momentum/param.disruption_off_axis.in index 0dfbae80a..831f310d5 100644 --- a/examples/symba_energy_momentum/param.disruption_off_axis.in +++ b/examples/symba_energy_momentum/param.disruption_off_axis.in @@ -1,15 +1,15 @@ T0 0.0e0 -TSTOP 0.000100 ! simulation length in seconds = 100 years +TSTOP 0.0001000 ! simulation length in seconds = 100 years DT 0.0000001 ! stepsize in seconds CB_IN cb.in PL_IN disruption_off_axis.in TP_IN tp.in IN_TYPE ASCII ISTEP_OUT 1 ! output cadence every year -BIN_OUT bin.disruption_off_axis.dat +BIN_OUT bin.disruption_off_axis.nc PARTICLE_OUT particle.disruption_off_axis.dat -OUT_TYPE REAL8 ! double precision real output -OUT_FORM XV ! osculating element output +OUT_TYPE NETCDF_DOUBLE ! double precision real output +OUT_FORM XVEL ! osculating element output OUT_STAT REPLACE ISTEP_DUMP 1 ! system dump cadence CHK_CLOSE yes ! check for planetary close encounters @@ -22,7 +22,8 @@ DISCARD_OUT discard.disruption_off_axis.out EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded RHILL_PRESENT yes ! Hill's sphere radii in input file -GMTINY 1.0e-16 +GMTINY 1.0e-11 +MIN_GMFRAG 1.0e-11 FRAGMENTATION yes MU2KG 1.98908e30 TU2S 3.1556925e7 diff --git a/examples/symba_energy_momentum/param.escape.in b/examples/symba_energy_momentum/param.escape.in index 90d118017..5f8ef2d0d 100644 --- a/examples/symba_energy_momentum/param.escape.in +++ b/examples/symba_energy_momentum/param.escape.in @@ -9,20 +9,16 @@ ISTEP_OUT 1 ! output cadence every year BIN_OUT bin.escape.dat PARTICLE_OUT particle.escape.dat OUT_TYPE REAL8 ! double precision real output -OUT_FORM XV ! osculating element output +OUT_FORM EL ! osculating element output OUT_STAT REPLACE ISTEP_DUMP 1 ! system dump cadence -J2 0.0 ! no J2 term -J4 0.0 ! no J4 term CHK_CLOSE yes ! check for planetary close encounters -CHK_RMIN 0.00465047 ! check for close solar encounters in AU CHK_RMAX 10000.0 ! discard outside of -CHK_EJECT -1.0 ! ignore this check -CHK_QMIN -1.0 ! ignore this check ENC_OUT enc.escape.dat +DISCARD_OUT discard.escape.dat EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded -RHILL_PRESENT no ! Hill's sphere radii in input file +RHILL_PRESENT yes ! Hill's sphere radii in input file GMTINY 1.0e-16 FRAGMENTATION yes MU2KG 1.98908e30 diff --git a/examples/symba_energy_momentum/param.hitandrun.in b/examples/symba_energy_momentum/param.hitandrun.in new file mode 100644 index 000000000..1e2e2eea7 --- /dev/null +++ b/examples/symba_energy_momentum/param.hitandrun.in @@ -0,0 +1,33 @@ +T0 0.0e0 +TSTOP 0.000100 ! simulation length in seconds = 100 years +DT 0.0000001 ! stepsize in seconds +CB_IN cb.in +PL_IN hitandrun.in +TP_IN tp.in +IN_TYPE ASCII +ISTEP_OUT 1 ! output cadence every year +BIN_OUT bin.hitandrun.nc +PARTICLE_OUT particle.hitandrun.dat +OUT_TYPE NETCDF_DOUBLE ! double precision real output +OUT_FORM XVEL ! osculating element output +OUT_STAT REPLACE +ISTEP_DUMP 1 ! system dump cadence +CHK_CLOSE yes ! check for planetary close encounters +CHK_RMIN 0.005 +CHK_RMAX 1e6 +CHK_EJECT -1.0 ! ignore this check +CHK_QMIN -1.0 ! ignore this check +ENC_OUT enc.hitandrun.dat +DISCARD_OUT discard.hitandrun.out +EXTRA_FORCE no ! no extra user-defined forces +BIG_DISCARD no ! output all planets if anything discarded +RHILL_PRESENT yes ! Hill's sphere radii in input file +GMTINY 1.0e-11 +MIN_GMFRAG 1.0e-11 +FRAGMENTATION yes +MU2KG 1.98908e30 +TU2S 3.1556925e7 +DU2M 1.49598e11 +ENERGY yes +ROTATION yes +SEED 8 933097 -220886113 -118730874 233084005 32111237 -823335422 524551114 -61162322 diff --git a/examples/symba_energy_momentum/param.sun.in b/examples/symba_energy_momentum/param.sun.in index a7748b19c..351d8adb2 100644 --- a/examples/symba_energy_momentum/param.sun.in +++ b/examples/symba_energy_momentum/param.sun.in @@ -19,15 +19,17 @@ CHK_RMIN 0.005 CHK_RMAX 1e2 CHK_EJECT -1.0 ! ignore this check CHK_QMIN -1.0 ! ignore this check -ENC_OUT enc.escape.dat +ENC_OUT enc.sun.dat +DISCARD_OUT discard.sun.dat EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded RHILL_PRESENT no ! Hill's sphere radii in input file GMTINY 1.0e-16 -FRAGMENTATION yes +FRAGMENTATION no MU2KG 1.98908e30 TU2S 3.1556925e7 DU2M 1.49598e11 ENERGY yes +ENERGY_OUT energy.sun.out ROTATION yes SEED 8 1230834 2346113 123409874 -123121105 -767545 -534058022 343309814 -12535638 diff --git a/examples/symba_energy_momentum/param.supercatastrophic_headon.in b/examples/symba_energy_momentum/param.supercatastrophic_headon.in index e9b60e7da..fd15c00dd 100644 --- a/examples/symba_energy_momentum/param.supercatastrophic_headon.in +++ b/examples/symba_energy_momentum/param.supercatastrophic_headon.in @@ -6,10 +6,10 @@ CB_IN cb.in TP_IN tp.in IN_TYPE ASCII ISTEP_OUT 1 ! output cadence every year -BIN_OUT bin.supercatastrophic_headon.dat +BIN_OUT bin.supercatastrophic_headon.nc PARTICLE_OUT particle.supercatastrophic_headon.dat -OUT_TYPE REAL8 ! double precision real output -OUT_FORM XV ! osculating element output +OUT_TYPE NETCDF_DOUBLE ! double precision real output +OUT_FORM XVEL ! osculating element output OUT_STAT REPLACE ISTEP_DUMP 1 ! system dump cadence CHK_CLOSE yes ! check for planetary close encounters @@ -17,11 +17,11 @@ CHK_RMIN 0.005 CHK_RMAX 1e6 CHK_EJECT -1.0 ! ignore this check CHK_QMIN -1.0 ! ignore this check -ENC_OUT enc.supercatastrophic_headon.dat EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded RHILL_PRESENT yes ! Hill's sphere radii in input file -GMTINY 1.0e-16 +GMTINY 1.0e-11 +MIN_GMFRAG 1.0e-11 FRAGMENTATION yes MU2KG 1.98908e30 TU2S 3.1556925e7 diff --git a/examples/symba_energy_momentum/param.supercatastrophic_off_axis.in b/examples/symba_energy_momentum/param.supercatastrophic_off_axis.in index 0bf836be5..51ab91e5d 100644 --- a/examples/symba_energy_momentum/param.supercatastrophic_off_axis.in +++ b/examples/symba_energy_momentum/param.supercatastrophic_off_axis.in @@ -21,7 +21,8 @@ ENC_OUT enc.supercatastrophic_off_axis.dat EXTRA_FORCE no ! no extra user-defined forces BIG_DISCARD no ! output all planets if anything discarded RHILL_PRESENT yes ! Hill's sphere radii in input file -GMTINY 1.0e-16 +GMTINY 1.0e-11 +MIN_GMFRAG 1.0e-11 FRAGMENTATION yes MU2KG 1.98908e30 TU2S 3.1556925e7 diff --git a/examples/symba_mars_disk/Untitled.ipynb b/examples/symba_mars_disk/Untitled.ipynb new file mode 100644 index 000000000..7fec51502 --- /dev/null +++ b/examples/symba_mars_disk/Untitled.ipynb @@ -0,0 +1,6 @@ +{ + "cells": [], + "metadata": {}, + "nbformat": 4, + "nbformat_minor": 4 +} diff --git a/examples/symba_mars_disk/aescattermovie.py b/examples/symba_mars_disk/aescattermovie.py new file mode 100755 index 000000000..85b99c0fa --- /dev/null +++ b/examples/symba_mars_disk/aescattermovie.py @@ -0,0 +1,125 @@ +#!/usr/bin/env python3 +import swiftest +import numpy as np +import matplotlib.pyplot as plt +from matplotlib import animation +import matplotlib.colors as mcolors + +titletext = "High M - High e" +radscale = 1000 +RMars = 3389500.0 +xmin = 1.0 +xmax = 10.0 +ymin = 1e-6 +ymax = 1.0 +framejump = 1 +ncutoff = 1e20 + +class AnimatedScatter(object): + """An animated scatter plot using matplotlib.animations.FuncAnimation.""" + def __init__(self, ds, param): + + frame = 0 + self.ds = ds + self.nframes = int(ds['time'].size / framejump) + self.Rcb = self.ds['radius'].sel(id=0, time=0).values + self.ds = ds + self.param = param + self.clist = {'Initial conditions' : 'xkcd:faded blue', + 'Disruption' : 'xkcd:marigold', + 'Supercatastrophic' : 'xkcd:shocking pink', + 'Hit and run fragment' : 'xkcd:baby poop green'} + + # Setup the figure and axes... + fig = plt.figure(figsize=(8,4.5), dpi=300) + plt.tight_layout(pad=0) + # set up the figure + self.ax = plt.Axes(fig, [0.1, 0.15, 0.8, 0.75]) + self.ax.set_xlim(xmin, xmax) + self.ax.set_ylim(ymin, ymax) + fig.add_axes(self.ax) + self.ani = animation.FuncAnimation(fig, self.update, interval=1, frames=self.nframes, init_func=self.setup_plot, blit=True) + #self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'libx264']) + self.ani.save('aescatter.mp4', fps=30, dpi=300, extra_args=['-vcodec', 'mpeg4']) + print('Finished writing aescattter.mp4') + + def scatters(self, pl, radmarker, origin): + scat = [] + for key, value in self.clist.items(): + idx = origin == key + s = self.ax.scatter(pl[idx, 0], pl[idx, 1], marker='o', s=radmarker[idx], c=value, alpha=0.75, label=key) + scat.append(s) + return scat + + def setup_plot(self): + # First frame + """Initial drawing of the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(0)) + + # set up the figure + self.ax.margins(x=10, y=1) + self.ax.set_xlabel('Semi Major Axis ($R_{Mars}$)', fontsize='16', labelpad=1) + self.ax.set_ylabel('Eccentricity', fontsize='16', labelpad=1) + self.ax.set_yscale('log') + + self.title = self.ax.text(0.50, 1.05, "", bbox={'facecolor': 'w', 'alpha': 0.5, 'pad': 5}, transform=self.ax.transAxes, + ha="center", animated=True) + + self.title.set_text(f"{titletext} - Time = ${t / 24 / 3600:4.1f}$ days with ${npl:f}$ particles") + slist = self.scatters(pl, radmarker, origin) + self.s0 = slist[0] + self.s1 = slist[1] + self.s2 = slist[2] + self.s3 = slist[3] + leg = plt.legend(loc="upper right", scatterpoints=1, fontsize=10) + for i,l in enumerate(leg.legendHandles): + leg.legendHandles[i]._sizes = [20] + return self.s0, self.s1, self.s2, self.s3, self.title + + def data_stream(self, frame=0): + while True: + d = self.ds.isel(time=frame) + + d = d.where(d['radius'] < self.Rcb, drop=True) + d['radmarker'] = (d['radius'] / self.Rcb) * radscale + radius = d['radmarker'].values + + Gmass = d['Gmass'].values + a = d['a'].values / self.Rcb + e = d['e'].values + name = d['name'].values + npl = d['npl'].values[0] + radmarker = d['radmarker'] + origin = d['origin_type'].values + + t = self.ds.coords['time'].values[frame] + + frame += 1 + yield t, name, Gmass, radius, npl, np.c_[a, e], radmarker, origin + + def update(self,frame): + """Update the scatter plot.""" + t, name, Gmass, radius, npl, pl, radmarker, origin = next(self.data_stream(framejump * frame)) + + self.title.set_text(f"{titletext} - Time = ${t / 24 / 3600:4.1f}$ days with ${npl:4.0f}$ particles") + + # We need to return the updated artist for FuncAnimation to draw.. + # Note that it expects a sequence of artists, thus the trailing comma. + s = [self.s0, self.s1, self.s2, self.s3] + for i, (key, value) in enumerate(self.clist.items()): + idx = origin == key + s[i].set_sizes(radmarker[idx]) + s[i].set_offsets(pl[idx,:]) + s[i].set_facecolor(value) + + self.s0 = s[0] + self.s1 = s[1] + self.s2 = s[2] + self.s3 = s[3] + return self.s0, self.s1, self.s2, self.s3, self.title, + +sim = swiftest.Simulation(param_file="param.in") +sim.bin2xr() +print('Making animation') +anim = AnimatedScatter(sim.ds,sim.param) +print('Animation finished') diff --git a/examples/symba_mars_disk/cb.in b/examples/symba_mars_disk/cb.in index c9dafacfd..6185284ec 100644 --- a/examples/symba_mars_disk/cb.in +++ b/examples/symba_mars_disk/cb.in @@ -1,4 +1,4 @@ -0 ! id +Mars ! name 4.28388662e+13 ! G*mass 3389500.0 ! radius 0.0 ! J2 diff --git a/examples/symba_mars_disk/mars.in b/examples/symba_mars_disk/mars.in index 8760a493d..188eb3c6e 100644 --- a/examples/symba_mars_disk/mars.in +++ b/examples/symba_mars_disk/mars.in @@ -1,9000 +1,9000 @@ 1500 ! Mars System in SI units -2 9.90685589e+04 8.35558297e+03 ! particle number mass Rhill -7.07643092e+03 !particle radius in m +Body2 9.90685589e+04 8.35558297e+03 ! particle number mass Rhill +7.07643092e+03 !particle radius in AU -2.35807426e+06 8.60445552e+06 1.25224401e+04 ! x y z -2.13373621e+03 -5.91159549e+02 -1.46482980e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -3 3.17438752e+04 6.69500494e+03 ! particle number mass Rhill -4.84234399e+03 !particle radius in m +Body3 3.17438752e+04 6.69500494e+03 ! particle number mass Rhill +4.84234399e+03 !particle radius in AU -8.01160007e+06 -6.93642997e+06 1.51456130e+04 ! x y z 1.31205897e+03 -1.53256580e+03 -1.41252951e-01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -4 3.98556011e+05 1.56022902e+04 ! particle number mass Rhill -1.12546530e+04 !particle radius in m +Body4 3.98556011e+05 1.56022902e+04 ! particle number mass Rhill +1.12546530e+04 !particle radius in AU 8.10802666e+05 1.07743901e+07 2.02908991e+04 ! x y z -1.97583939e+03 1.47020293e+02 2.81847341e-01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -5 1.44988335e+05 1.52187807e+04 ! particle number mass Rhill -5.45209420e+03 !particle radius in m +Body5 1.44988335e+05 1.52187807e+04 ! particle number mass Rhill +5.45209420e+03 !particle radius in AU 1.19634122e+07 -8.10716246e+06 -5.95532256e+04 ! x y z 9.82512278e+02 1.42576317e+03 8.88854207e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -6 3.78500932e+05 1.43710361e+04 ! particle number mass Rhill -7.50714229e+03 !particle radius in m +Body6 3.78500932e+05 1.43710361e+04 ! particle number mass Rhill +7.50714229e+03 !particle radius in AU -9.39611249e+06 3.86341011e+06 4.12677461e+04 ! x y z -8.05714130e+02 -1.87378063e+03 1.44571432e+01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -7 4.22792487e+05 1.91833939e+04 ! particle number mass Rhill -7.78923399e+03 !particle radius in m +Body7 4.22792487e+05 1.91833939e+04 ! particle number mass Rhill +7.78923399e+03 !particle radius in AU -4.75251420e+06 -1.21243281e+07 -4.63584868e+04 ! x y z 1.67483168e+03 -6.72935315e+02 -2.51894419e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -8 7.71745838e+05 2.46689817e+04 ! particle number mass Rhill -9.51941869e+03 !particle radius in m +Body8 7.71745838e+05 2.46689817e+04 ! particle number mass Rhill +9.51941869e+03 !particle radius in AU -1.85450966e+06 -1.34716389e+07 8.25492639e+04 ! x y z 1.75187299e+03 -2.73602528e+02 -3.13786565e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -9 9.61893115e+05 2.40394481e+04 ! particle number mass Rhill -1.02445905e+04 !particle radius in m +Body9 9.61893115e+05 2.40394481e+04 ! particle number mass Rhill +1.02445905e+04 !particle radius in AU 1.23514674e+07 2.68920661e+05 1.39262437e+04 ! x y z -5.46299990e+01 1.85637492e+03 8.88156878e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -10 9.05777402e+05 1.85084324e+04 ! particle number mass Rhill -1.00413666e+04 !particle radius in m +Body10 9.05777402e+05 1.85084324e+04 ! particle number mass Rhill +1.00413666e+04 !particle radius in AU -3.23931710e+06 -9.01689172e+06 -4.12799209e+04 ! x y z 2.01018172e+03 -6.80970287e+02 7.47887585e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -11 7.45490873e+05 1.85936744e+04 ! particle number mass Rhill -9.41021993e+03 !particle radius in m +Body11 7.45490873e+05 1.85936744e+04 ! particle number mass Rhill +9.41021993e+03 !particle radius in AU -8.22383274e+06 6.53912283e+06 -4.14927827e+04 ! x y z -1.24361728e+03 -1.57101590e+03 1.15408315e+01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -12 1.62561944e+05 1.74719338e+04 ! particle number mass Rhill -5.66402670e+03 !particle radius in m +Body12 1.62561944e+05 1.74719338e+04 ! particle number mass Rhill +5.66402670e+03 !particle radius in AU 1.08162501e+06 1.60434368e+07 -1.90513596e+05 ! x y z -1.63320995e+03 9.41371249e+01 -1.08583324e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -13 2.53914705e+05 1.18629878e+04 ! particle number mass Rhill -9.68422654e+03 !particle radius in m +Body13 2.53914705e+05 1.18629878e+04 ! particle number mass Rhill +9.68422654e+03 !particle radius in AU 8.87638562e+06 -3.42494393e+06 3.77051239e+04 ! x y z 7.17031490e+02 1.98991002e+03 1.65715407e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -14 4.49497062e+05 1.80709533e+04 ! particle number mass Rhill -1.17150625e+04 !particle radius in m +Body14 4.49497062e+05 1.80709533e+04 ! particle number mass Rhill +1.17150625e+04 !particle radius in AU 8.43240423e+06 -8.47557599e+06 9.53685695e+04 ! x y z 1.37244856e+03 1.29766742e+03 6.52389482e-01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -15 1.26801801e+06 2.59747860e+04 ! particle number mass Rhill -1.12329581e+04 !particle radius in m +Body15 1.26801801e+06 2.59747860e+04 ! particle number mass Rhill +1.12329581e+04 !particle radius in AU 9.22664947e+06 8.30989011e+06 -5.74831096e+04 ! x y z -1.25111883e+03 1.34059241e+03 8.55955292e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -16 9.75352347e+05 2.91597894e+04 ! particle number mass Rhill -1.02921516e+04 !particle radius in m +Body16 9.75352347e+05 2.91597894e+04 ! particle number mass Rhill +1.02921516e+04 !particle radius in AU -4.08982641e+06 1.42813091e+07 2.62466604e+04 ! x y z -1.63050329e+03 -4.70983328e+02 5.42658810e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -17 5.40910752e+04 7.00056187e+03 ! particle number mass Rhill -3.92489041e+03 !particle radius in m +Body17 5.40910752e+04 7.00056187e+03 ! particle number mass Rhill +3.92489041e+03 !particle radius in AU 8.28836769e+06 -4.56966319e+06 -1.00925184e+04 ! x y z 1.01075458e+03 1.85603564e+03 9.12767608e-01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -18 1.99689612e+06 3.23933078e+04 ! particle number mass Rhill -1.30688534e+04 !particle radius in m +Body18 1.99689612e+06 3.23933078e+04 ! particle number mass Rhill +1.30688534e+04 !particle radius in AU -7.36104027e+06 -1.05891946e+07 7.75267384e+04 ! x y z 1.50650168e+03 -1.03626339e+03 6.92830281e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -19 1.15056094e+06 2.84099265e+04 ! particle number mass Rhill -1.08748232e+04 !particle radius in m +Body19 1.15056094e+06 2.84099265e+04 ! particle number mass Rhill +1.08748232e+04 !particle radius in AU -1.16432549e+07 7.04896042e+06 1.31826777e+04 ! x y z -9.22639859e+02 -1.52066967e+03 -1.15982407e+01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -20 9.02282771e+04 1.44052969e+04 ! particle number mass Rhill -4.65478777e+03 !particle radius in m +Body20 9.02282771e+04 1.44052969e+04 ! particle number mass Rhill +4.65478777e+03 !particle radius in AU 1.54278872e+07 -4.66477914e+06 2.89150511e+04 ! x y z 4.74802657e+02 1.56436208e+03 1.16558658e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -21 2.52706341e+05 1.13089015e+04 ! particle number mass Rhill -6.56131734e+03 !particle radius in m +Body21 2.52706341e+05 1.13089015e+04 ! particle number mass Rhill +6.56131734e+03 !particle radius in AU 8.25405514e+06 -3.99894087e+06 -1.03017471e+05 ! x y z 9.55530709e+02 1.91876743e+03 -2.12478228e+01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -22 3.44014800e+05 1.39895248e+04 ! particle number mass Rhill -7.27184654e+03 !particle radius in m +Body22 3.44014800e+05 1.39895248e+04 ! particle number mass Rhill +7.27184654e+03 !particle radius in AU -1.01048660e+07 -7.25267430e+05 3.72763878e+04 ! x y z 1.50338830e+02 -2.04513843e+03 -6.64737882e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -23 2.72301402e+04 6.52734935e+03 ! particle number mass Rhill -4.60100051e+03 !particle radius in m +Body23 2.72301402e+04 6.52734935e+03 ! particle number mass Rhill +4.60100051e+03 !particle radius in AU 1.08085981e+07 8.91343848e+05 -8.59837690e+04 ! x y z -1.73598988e+02 1.98921090e+03 7.39675166e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -24 1.88387060e+06 4.79739567e+04 ! particle number mass Rhill -1.28174811e+04 !particle radius in m +Body24 1.88387060e+06 4.79739567e+04 ! particle number mass Rhill +1.28174811e+04 !particle radius in AU -1.95760874e+07 2.13874411e+06 9.87141675e+04 ! x y z -1.78019032e+02 -1.46067517e+03 7.47552271e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -25 1.99552106e+06 3.51994254e+04 ! particle number mass Rhill -1.30658530e+04 !particle radius in m +Body25 1.99552106e+06 3.51994254e+04 ! particle number mass Rhill +1.30658530e+04 !particle radius in AU -5.15587895e+06 1.31093030e+07 2.34999443e+04 ! x y z -1.60915655e+03 -6.75665775e+02 -1.41401807e-02 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -26 9.80460627e+05 2.82973543e+04 ! particle number mass Rhill -1.03100883e+04 !particle radius in m +Body26 9.80460627e+05 2.82973543e+04 ! particle number mass Rhill +1.03100883e+04 !particle radius in AU -1.04206598e+07 1.04694469e+07 3.71773715e+04 ! x y z -1.22193412e+03 -1.15184993e+03 -7.42970615e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -27 2.99657072e+05 1.52153060e+04 ! particle number mass Rhill -1.02339628e+04 !particle radius in m +Body27 2.99657072e+05 1.52153060e+04 ! particle number mass Rhill +1.02339628e+04 !particle radius in AU -8.37104048e+06 -7.31013791e+06 1.37822827e+05 ! x y z 1.31083458e+03 -1.50225202e+03 1.24188931e+01 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -28 5.82137831e+05 2.49711445e+04 ! particle number mass Rhill -8.66551286e+03 !particle radius in m +Body28 5.82137831e+05 2.49711445e+04 ! particle number mass Rhill +8.66551286e+03 !particle radius in AU -1.37026179e+07 6.52187486e+06 4.74483726e+04 ! x y z -7.21171063e+02 -1.51233609e+03 4.06777653e+00 ! vx vy vz 0.4 0.4 0.4 ! Ip 0.0 0.0 0.0 ! rot -29 1.10612525e+06 1.96262714e+04 ! particle number mass Rhill -1.07329828e+04 !particle radius in m +Body29 1.10612525e+06 1.96262714e+04 ! particle number mass Rhill +1.07329828e+04 !particle radius in AU 7.27063487e+05 9.63835599e+06 7.97365647e+04 ! x y z -2.09031891e+03 1.45245810e+02 -8.30488647e+00 ! vx vy vz 0.4 0.4 0.4 ! 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}, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.7.10" + } + }, + "nbformat": 4, + "nbformat_minor": 4 +} diff --git a/examples/symba_mars_disk/timetest.sh b/examples/symba_mars_disk/timetest.sh new file mode 100755 index 000000000..e881f6ceb --- /dev/null +++ b/examples/symba_mars_disk/timetest.sh @@ -0,0 +1,9 @@ +#!/bin/bash +outname="timetest.csv" +echo "N cores, wall time (s)" > $outname +for value in {1..12} +do + export OMP_NUM_THREADS=$value + walltime="$(/usr/bin/time -f %e ./swiftest_driver symba param.in 2>&1 > /dev/null)" + echo "$value,$walltime" >> $outname +done \ No newline at end of file diff --git a/examples/symba_mars_disk/tp.in b/examples/symba_mars_disk/tp.in index 573541ac9..c22708346 100644 --- a/examples/symba_mars_disk/tp.in +++ b/examples/symba_mars_disk/tp.in @@ -1 +1 @@ -0 +0 \ No newline at end of file diff --git a/examples/symba_swifter_comparison/1pl_1pl_encounter/init_cond.py b/examples/symba_swifter_comparison/1pl_1pl_encounter/init_cond.py index 6547c2802..328ed30c9 100755 --- a/examples/symba_swifter_comparison/1pl_1pl_encounter/init_cond.py +++ b/examples/symba_swifter_comparison/1pl_1pl_encounter/init_cond.py @@ -59,8 +59,8 @@ p_pl2 = np.array([apl2, 0.0, 0.0], dtype=np.double) v_pl2 = np.array([0.0, vpl2, 0.0], dtype=np.double) -Rhill1 = np.double(apl1 * 0.0100447248332378922085) -Rhill2 = Rhill1 * (mass2 / mass1)**(1.0 / 3.0) +rhill1 = np.double(apl1 * 0.0100447248332378922085) +rhill2 = rhill1 * (mass2 / mass1)**(1.0 / 3.0) #Make Swifter files plfile = open(swifter_pl, 'w') @@ -70,12 +70,12 @@ print('0.0 0.0 0.0',file=plfile) print('0.0 0.0 0.0',file=plfile) -print(plid1,"{:.23g}".format(mass1),Rhill1, file=plfile) +print(plid1,"{:.23g}".format(mass1),rhill1, file=plfile) print(radius1, file=plfile) print(*p_pl1, file=plfile) print(*v_pl1, file=plfile) -print(plid2,"{:.23g}".format(mass2),Rhill2, file=plfile) +print(plid2,"{:.23g}".format(mass2),rhill2, file=plfile) print(radius2, file=plfile) print(*p_pl2, file=plfile) print(*v_pl2, file=plfile) @@ -139,7 +139,7 @@ plfile.write_record(np.vstack([v_pl1[1],v_pl2[1]])) plfile.write_record(np.vstack([v_pl1[2],v_pl2[2]])) plfile.write_record(np.array([mass1,mass2])) -plfile.write_record(np.array([Rhill1,Rhill2])) +plfile.write_record(np.array([rhill1,rhill2])) plfile.write_record(np.array([radius1,radius2])) plfile.close() tpfile = FortranFile(swiftest_tp, 'w') diff --git a/examples/symba_swifter_comparison/1pl_1pl_encounter/param.swifter.in b/examples/symba_swifter_comparison/1pl_1pl_encounter/param.swifter.in index 853815639..a67348c0e 100644 --- a/examples/symba_swifter_comparison/1pl_1pl_encounter/param.swifter.in +++ b/examples/symba_swifter_comparison/1pl_1pl_encounter/param.swifter.in @@ -24,3 +24,4 @@ ENC_OUT enc.swifter.dat EXTRA_FORCE no BIG_DISCARD no RHILL_PRESENT yes +ENERGY yes diff --git a/examples/symba_swifter_comparison/1pl_1pl_encounter/swiftest_vs_swifter.ipynb b/examples/symba_swifter_comparison/1pl_1pl_encounter/swiftest_vs_swifter.ipynb index 3a80eebd1..6c5bc45e4 100644 --- a/examples/symba_swifter_comparison/1pl_1pl_encounter/swiftest_vs_swifter.ipynb +++ b/examples/symba_swifter_comparison/1pl_1pl_encounter/swiftest_vs_swifter.ipynb @@ -2,7 +2,7 @@ "cells": [ { "cell_type": "code", - "execution_count": 8, + "execution_count": 1, "metadata": {}, "outputs": [], "source": [ @@ -13,7 +13,7 @@ }, { "cell_type": "code", - "execution_count": 9, + "execution_count": 2, "metadata": {}, "outputs": [ { @@ -35,7 +35,7 @@ }, { "cell_type": "code", - "execution_count": 10, + "execution_count": 3, "metadata": {}, "outputs": [ { @@ -57,7 +57,7 @@ }, { "cell_type": "code", - "execution_count": 11, + "execution_count": 4, "metadata": {}, "outputs": [], "source": [ @@ -66,7 +66,7 @@ }, { "cell_type": "code", - "execution_count": 12, + "execution_count": 5, "metadata": {}, "outputs": [], "source": [ @@ -75,23 +75,23 @@ }, { "cell_type": "code", - "execution_count": 13, + "execution_count": 6, "metadata": {}, "outputs": [ { "data": { "text/plain": [ - "[,\n", - " ]" + "[,\n", + " ]" ] }, - "execution_count": 13, + "execution_count": 6, "metadata": {}, "output_type": "execute_result" }, { "data": { - "image/png": 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\n", 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\n", 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" ] @@ -106,1512 +106,6 @@ "swiftdiff['vx'].plot.line(x=\"time (y)\")" ] }, - { - "cell_type": "code", - "execution_count": 19, - "metadata": {}, - "outputs": [ - { - "data": { - "text/html": [ - "
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"cell_type": "code", "execution_count": null, diff --git a/examples/symba_swifter_comparison/1pl_1tp_encounter/init_cond.py b/examples/symba_swifter_comparison/1pl_1tp_encounter/init_cond.py index ac55abb2b..b516bda9c 100755 --- a/examples/symba_swifter_comparison/1pl_1tp_encounter/init_cond.py +++ b/examples/symba_swifter_comparison/1pl_1tp_encounter/init_cond.py @@ -59,7 +59,7 @@ p_tp = np.array([atp, 0.0, 0.0], dtype=np.double) v_tp = np.array([0.0, vtp, 0.0], dtype=np.double) -Rhill = np.double(apl * 0.0100447248332378922085) +rhill = np.double(apl * 0.0100447248332378922085) #Make Swifter files plfile = open(swifter_pl, 'w') @@ -67,7 +67,7 @@ print(1,GMSun,file=plfile) print('0.0 0.0 0.0',file=plfile) print('0.0 0.0 0.0',file=plfile) -print(plid,"{:.23g}".format(mass),Rhill, file=plfile) +print(plid,"{:.23g}".format(mass),rhill, file=plfile) print(radius, file=plfile) print(*p_pl, file=plfile) print(*v_pl, file=plfile) @@ -130,7 +130,7 @@ plfile.write_record(v_pl[1]) plfile.write_record(v_pl[2]) plfile.write_record(mass) -plfile.write_record(Rhill) +plfile.write_record(rhill) plfile.write_record(radius) plfile.close() tpfile = FortranFile(swiftest_tp, 'w') diff --git a/examples/symba_swifter_comparison/8pl_16tp_encounters/init_cond.py b/examples/symba_swifter_comparison/8pl_16tp_encounters/init_cond.py index 546dcbb88..7ab52fd23 100755 --- a/examples/symba_swifter_comparison/8pl_16tp_encounters/init_cond.py +++ b/examples/symba_swifter_comparison/8pl_16tp_encounters/init_cond.py @@ -85,16 +85,16 @@ for i in pl.id: pli = pl.sel(id=i) - rstart = 2 * np.double(pli['Radius']) # Start the test particles at a multiple of the planet radius away + rstart = 2 * np.double(pli['radius']) # Start the test particles at a multiple of the planet radius away vstart = 1.5 * np.sqrt(2 * np.double(pli['Mass']) / rstart) # Start the test particle velocities at a multiple of the escape speed xvstart = np.array([rstart / np.sqrt(2.0), rstart / np.sqrt(2.0), 0.0, vstart, 0.0, 0.0]) # The positions and velocities of each pair of test particles will be in reference to a planet - plvec = np.array([np.double(pli['px']), - np.double(pli['py']), - np.double(pli['pz']), - np.double(pli['vx']), - np.double(pli['vy']), - np.double(pli['vz'])]) + plvec = np.array([np.double(pli['xhx']), + np.double(pli['xhy']), + np.double(pli['xhz']), + np.double(pli['vhx']), + np.double(pli['vhy']), + np.double(pli['vhz'])]) tpxv1 = plvec + xvstart tpxv2 = plvec - xvstart p1.append(tpxv1[0]) diff --git a/examples/symba_swifter_comparison/8pl_16tp_encounters/swiftest_symba_vs_swifter_symba.ipynb b/examples/symba_swifter_comparison/8pl_16tp_encounters/swiftest_symba_vs_swifter_symba.ipynb index 76094351b..ca5040a17 100644 --- a/examples/symba_swifter_comparison/8pl_16tp_encounters/swiftest_symba_vs_swifter_symba.ipynb +++ b/examples/symba_swifter_comparison/8pl_16tp_encounters/swiftest_symba_vs_swifter_symba.ipynb @@ -163,7 +163,7 @@ }, { "data": { - "image/png": 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\n", 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\n", 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\n", 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\n", "text/plain": [ "
" ] @@ -587,28 +587,18 @@ " stroke: currentColor;\n", " fill: currentColor;\n", "}\n", - "
<xarray.DataArray 'px' (id: 16)>\n",
-       "array([ 0.0000000e+00,  0.0000000e+00,  4.4408921e-16,  0.0000000e+00,\n",
-       "        0.0000000e+00, -4.4408921e-16,  4.4408921e-16,  0.0000000e+00,\n",
-       "        0.0000000e+00,  0.0000000e+00,  0.0000000e+00,  0.0000000e+00,\n",
-       "        0.0000000e+00,  0.0000000e+00,  0.0000000e+00,  0.0000000e+00])\n",
+       "
<xarray.DataArray 'px' (id: 8)>\n",
+       "array([0., 0., 0., 0., 0., 0., 0., 0.])\n",
        "Coordinates:\n",
-       "  * id       (id) int64 101 102 103 104 105 106 107 ... 111 112 113 114 115 116\n",
-       "    time     float64 110.0
"
+       "  * id       (id) int64 1 2 3 4 5 6 7 8\n",
+       "    time     float64 11.0
" ], "text/plain": [ - "\n", - "array([ 0.0000000e+00, 0.0000000e+00, 4.4408921e-16, 0.0000000e+00,\n", - " 0.0000000e+00, -4.4408921e-16, 4.4408921e-16, 0.0000000e+00,\n", - " 0.0000000e+00, 0.0000000e+00, 0.0000000e+00, 0.0000000e+00,\n", - " 0.0000000e+00, 0.0000000e+00, 0.0000000e+00, 0.0000000e+00])\n", + "\n", + "array([0., 0., 0., 0., 0., 0., 0., 0.])\n", "Coordinates:\n", - " * id (id) int64 101 102 103 104 105 106 107 ... 111 112 113 114 115 116\n", - " time float64 110.0" + " * id (id) int64 1 2 3 4 5 6 7 8\n", + " time float64 11.0" ] }, "execution_count": 13, @@ -617,7 +607,7 @@ } ], "source": [ - "swiftdiff['px'].sel(id=tpidx).isel(time=10)" + "swiftdiff['px'].sel(id=plidx).isel(time=1)" ] }, { diff --git a/examples/symba_swifter_comparison/mars_disk/cb.in b/examples/symba_swifter_comparison/mars_disk/cb.in new file mode 100644 index 000000000..c9dafacfd --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/cb.in @@ -0,0 +1,7 @@ +0 ! id +4.28388662e+13 ! G*mass +3389500.0 ! radius +0.0 ! J2 +0.0 ! J4 +0.4 0.4 0.4 ! Ip +0.0 0.0 0.0 ! rot diff --git a/examples/symba_swifter_comparison/mars_disk/param.swifter.in b/examples/symba_swifter_comparison/mars_disk/param.swifter.in new file mode 100644 index 000000000..79e415a10 --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/param.swifter.in @@ -0,0 +1,27 @@ +T0 0.0 +TSTOP 4200.0 +DT 600.0 +PL_IN pl.swifter.in +TP_IN tp.in +IN_TYPE ASCII +ISTEP_OUT 1 +ISTEP_DUMP 1 +BIN_OUT bin.swifter.dat +OUT_TYPE REAL8 +OUT_FORM XV +OUT_STAT UNKNOWN +J2 0.0 +J4 0.0 +CHK_CLOSE yes +CHK_RMIN 3389500.0 +CHK_RMAX 3389500000.0 +CHK_EJECT 3389500000.0 +CHK_QMIN 3389500.0 +CHK_QMIN_COORD HELIO +CHK_QMIN_RANGE 3389500.0 338950000000.0 +ENC_OUT /dev/null +EXTRA_FORCE no +BIG_DISCARD no +RHILL_PRESENT yes +WALLTIME yes +ENERGY yes diff --git a/examples/symba_swifter_comparison/mars_disk/param.swiftest.in b/examples/symba_swifter_comparison/mars_disk/param.swiftest.in new file mode 100644 index 000000000..e36498f4b --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/param.swiftest.in @@ -0,0 +1,33 @@ +!Parameter file for the SyMBA-RINGMOONS test +T0 0.0 +TSTOP 4200.0 +DT 600.0 +PL_IN pl.swiftest.in +TP_IN tp.in +IN_TYPE ASCII +ISTEP_OUT 1 +ISTEP_DUMP 1 +BIN_OUT bin.swiftest.dat +PARTICLE_OUT particle.dat +OUT_TYPE REAL8 +OUT_FORM XV +OUT_STAT REPLACE +CHK_CLOSE yes +CHK_RMIN 3389500.0 +CHK_RMAX 3389500000.0 +CHK_EJECT 3389500000.0 +CHK_QMIN 3389500.0 +CHK_QMIN_COORD HELIO +CHK_QMIN_RANGE 3389500.0 338950000000.0 +EXTRA_FORCE no +BIG_DISCARD no +RHILL_PRESENT yes +GMTINY 1000.0 +ENERGY yes +ENERGY_OUT energy.dat +FRAGMENTATION yes +ROTATION yes +MU2KG 1.0 +DU2M 1.0 +TU2S 1.0 +SEED 2 3080983 2220830 diff --git a/examples/symba_swifter_comparison/mars_disk/pl.swifter.in b/examples/symba_swifter_comparison/mars_disk/pl.swifter.in new file mode 100644 index 000000000..4c31c52c1 --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/pl.swifter.in @@ -0,0 +1,6004 @@ +1501 ! 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x y z +-1.74178290e+03 -1.18522553e+03 2.27430689e+00 ! vx vy vz diff --git a/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in b/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in new file mode 100644 index 000000000..72a58d839 --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in @@ -0,0 +1,9001 @@ +1500 ! 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Ip +0.0 0.0 0.0 ! rot diff --git a/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb b/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb new file mode 100644 index 000000000..1dca7f7e8 --- /dev/null +++ b/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb @@ -0,0 +1,516 @@ +{ + "cells": [ + { + "cell_type": "code", + "execution_count": 1, + "metadata": {}, + "outputs": [], + "source": [ + "import numpy as np\n", + "import swiftest\n", + "import matplotlib.pyplot as plt" + ] + }, + { + "cell_type": "code", + "execution_count": 2, + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Reading Swifter file param.swifter.in\n", + "Reading in time 4.200e+03\n", + "Creating Dataset\n", + "Successfully converted 8 output frames.\n", + "Swifter simulation data stored as xarray DataSet .ds\n" + ] + } + ], + "source": [ + "swiftersim = swiftest.Simulation(param_file=\"param.swifter.in\", codename=\"Swifter\")\n", + "swiftersim.bin2xr()" + ] + }, + { + "cell_type": "code", + "execution_count": 3, + "metadata": {}, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Reading Swiftest file param.swiftest.in\n", + "Reading in time 0.000e+00\n", + "Creating Dataset\n", + "Successfully converted 1 output frames.\n", + "\n", + "Adding particle info to Dataset\n", + "Swiftest simulation data stored as xarray DataSet .ds\n" + ] + } + ], + "source": [ + "swiftestsim = swiftest.Simulation(param_file=\"param.swiftest.in\")\n", + "swiftestsim.bin2xr()" + ] + }, + { + "cell_type": "code", + "execution_count": 8, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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" ] }, - "metadata": { - "needs_background": "light" - }, + "metadata": {}, "output_type": "display_data" } ], "source": [ - "fig, ax = plt.subplots()\n", - "\n", - "ax.plot(t, varpi_obs, label=\"JPL Horizons\")\n", - "ax.plot(tsim, varpiswifter, label=\"Swifter GR\")\n", - "ax.plot(tsim, varpiswiftest, label=\"Swiftest GR\")\n", - "ax.set_xlabel('Time (y)')\n", - "ax.set_ylabel('Mercury $\\\\varpi$ (deg)')\n", - "ax.legend()\n", + "axes_fontsize = 32\n", + "legend_fontsize = 24\n", + "CB_color_cycle = ['#377eb8', '#ff7f00', '#4daf4a',\n", + " '#f781bf', '#a65628', '#984ea3',\n", + " '#999999', '#e41a1c', '#dede00']\n", + "fig = plt.figure(1, figsize=(14,10), facecolor=\"white\")\n", + "ax = fig.add_subplot(111)\n", + "plt.setp(ax.get_xticklabels(), fontsize=axes_fontsize)\n", + "plt.setp(ax.get_yticklabels(), fontsize=axes_fontsize)\n", + "ax.plot(t, varpi_obs, label=\"JPL Horizons\", linestyle='-',linewidth=6,c=CB_color_cycle[1])\n", + "ax.plot(tsim, varpinogr, label=\"Swiftest WHM No GR\", linestyle='--', linewidth=6, c=CB_color_cycle[0])\n", + "ax.plot(tsim, varpiswiftest, label=\"Swiftest WHM GR\", linestyle=':', linewidth=6,c=CB_color_cycle[2])\n", + "ax.set_xlabel(\"Time (y)\", fontsize=axes_fontsize)\n", + "ax.set_ylabel(\"Mercury $\\\\varpi$ (deg)\", fontsize=axes_fontsize)\n", + "ax.legend(loc=\"upper left\", fontsize=legend_fontsize, markerscale=1)\n", "print('Mean precession rate for Mercury long. peri. (arcsec/100 y)')\n", - "print(f'JPL Horizons : {np.mean(dvarpi_obs)}')\n", - "print(f'Swifter GR : {np.mean(dvarpi_swifter)}')\n", - "print(f'Swiftest GR : {np.mean(dvarpi_swiftest)}')\n", - "print(f'Obs - Swifter : {np.mean(dvarpi_obs - dvarpi_swifter)}')\n", - "print(f'Obs - Swiftest : {np.mean(dvarpi_obs - dvarpi_swiftest)}')\n", - "print(f'Swiftest - Swifter: {np.mean(dvarpi_swiftest - dvarpi_swifter)}')" + "print(f'Swiftest WHM No GR : {np.mean(dvarpi_nogr)}')\n", + "print(f'Swiftest WHM GR : {np.mean(dvarpi_swiftest)}')\n", + "print(f'JPL Horizons : {np.mean(dvarpi_obs)}')\n", + "print(f'Obs - Swiftest No GR : {np.mean(dvarpi_obs - dvarpi_nogr)}')\n", + "print(f'Obs - Swiftest GR : {np.mean(dvarpi_obs - dvarpi_swiftest)}')\n" ] }, { @@ -160,6 +189,13 @@ "outputs": [], "source": [] }, + { + "cell_type": "code", + "execution_count": null, + "metadata": {}, + "outputs": [], + "source": [] + }, { "cell_type": "code", "execution_count": null, diff --git a/python/swiftest/swiftest/constants.py b/python/swiftest/swiftest/constants.py index 7b031b4b7..caf8f8fe7 100644 --- a/python/swiftest/swiftest/constants.py +++ b/python/swiftest/swiftest/constants.py @@ -13,3 +13,4 @@ # Solar oblatenes values: From Mecheri et al. (2004), using Corbard (b) 2002 values (Table II) J2Sun = np.longdouble(2.198e-7) J4Sun = np.longdouble(-4.805e-9) + diff --git a/python/swiftest/swiftest/init_cond.py b/python/swiftest/swiftest/init_cond.py index f9a7378c0..12f0ef6ed 100644 --- a/python/swiftest/swiftest/init_cond.py +++ b/python/swiftest/swiftest/init_cond.py @@ -1,6 +1,8 @@ import swiftest import numpy as np from astroquery.jplhorizons import Horizons +import astropy.units as u +from astropy.coordinates import SkyCoord import datetime from datetime import date import xarray as xr @@ -74,6 +76,32 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): 'Pluto': np.longdouble(1188.3e3 / swiftest.AU2M) } + planetrot = { + 'Sun' : np.longdouble(2*np.pi / 25.05) / swiftest.JD2S, # Approximate + 'Mercury': np.longdouble(2*np.pi / 58.646) / swiftest.JD2S, + 'Venus': np.longdouble(2*np.pi / 243.0226 ) / swiftest.JD2S, + 'Earth': np.longdouble(2*np.pi / 0.99726968) / swiftest.JD2S, + 'Mars': np.longdouble(2*np.pi / 1.025957) / swiftest.JD2S, + 'Jupiter': np.longdouble(2*np.pi / (9.9250 / 24.0) ) / swiftest.JD2S, + 'Saturn': np.longdouble(2*np.pi / (10.656 / 24.0) ) / swiftest.JD2S, + 'Uranus': np.longdouble(2*np.pi / 0.71833) / swiftest.JD2S, + 'Neptune': np.longdouble(2*np.pi / 0.6713) / swiftest.JD2S, + 'Pluto': np.longdouble(2*np.pi / 6.387230) / swiftest.JD2S + } + + planetIpz = { # Only the polar moments of inertia are used currently. Where the quantity is unkown, we just use the value of a sphere = 0.4 + 'Sun' : np.longdouble(0.070), + 'Mercury' : np.longdouble(0.346), + 'Venus': np.longdouble(0.4), + 'Earth': np.longdouble(0.3307), + 'Mars': np.longdouble(0.3644), + 'Jupiter': np.longdouble(0.2756), + 'Saturn': np.longdouble(0.22), + 'Uranus': np.longdouble(0.23), + 'Neptune': np.longdouble(0.23), + 'Pluto': np.longdouble(0.4) + } + # Unit conversion factors DCONV = swiftest.AU2M / param['DU2M'] VCONV = (swiftest.AU2M / swiftest.JD2S) / (param['DU2M'] / param['TU2S']) @@ -84,8 +112,16 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): Rcb = np.array([swiftest.RSun / param['DU2M']]) J2RP2 = np.array([swiftest.J2Sun * (swiftest.RSun / param['DU2M']) ** 2]) J4RP4 = np.array([swiftest.J4Sun * (swiftest.RSun / param['DU2M']) ** 4]) + + solarpole = SkyCoord(ra=286.13 * u.degree, dec=63.87 * u.degree) + solarrot = planetrot['Sun'] * param['TU2S'] + rotcb = solarpole.cartesian * solarrot + Ipsun = np.array([0.0, 0.0, planetIpz['Sun']]) + cbid = np.array([0]) cvec = np.vstack([GMcb, Rcb, J2RP2, J4RP4]) + if param['ROTATION'] == 'YES': + cvec = np.vstack([cvec, Ipsun[0], Ipsun[1], Ipsun[2], rotcb.x, rotcb.y, rotcb.z]) # Horizons date time internal variables tstart = datetime.date.fromisoformat(ephemerides_start_date) @@ -95,6 +131,7 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): ephemerides_step = '1d' clab, plab, tlab = swiftest.io.make_swiftest_labels(param) + # Add the missing labels if param['OUT_FORM'] == 'XV': plab.append('a') plab.append('e') @@ -109,18 +146,18 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): tlab.append('omega') tlab.append('capm') elif param['OUT_FORM'] == 'EL': - plab.append('px') - plab.append('py') - plab.append('pz') - plab.append('vx') - plab.append('vy') - plab.append('vz') - tlab.append('px') - tlab.append('py') - tlab.append('pz') - tlab.append('vx') - tlab.append('vy') - tlab.append('vz') + plab.append('xhx') + plab.append('xhy') + plab.append('xhz') + plab.append('vhx') + plab.append('vhy') + plab.append('vhz') + tlab.append('xhx') + tlab.append('xhy') + tlab.append('xhz') + tlab.append('vhx') + tlab.append('vhy') + tlab.append('vhz') dims = ['time', 'id', 'vec'] t = np.array([0.0]) @@ -132,14 +169,14 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): val = -1 if key == "Sun" : # Create central body print("Creating the Sun as a central body") - cb = [] cbframe = np.expand_dims(cvec.T, axis=0) cbxr = xr.DataArray(cbframe, dims=dims, coords={'time': t, 'id': cbid, 'vec': clab}) + cbxr = cbxr.assign_coords(name=('id', [key])) cbds = cbxr.to_dataset(dim='vec') ds = xr.combine_by_coords([ds, cbds]) else: # Fetch solar system ephemerides from Horizons print(f"Fetching ephemerides data for {key} from JPL/Horizons") - pl = [] + p1 = [] p2 = [] p3 = [] @@ -152,9 +189,15 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): p10 = [] p11 = [] p12 = [] - Rhill = [] + rhill = [] Rpl = [] GMpl = [] + Ip1 = [] + Ip2 = [] + Ip3 = [] + rotx = [] + roty = [] + rotz = [] pldata = {} if ispl: @@ -165,7 +208,7 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): pldata[key] = Horizons(id=key, id_type='smallbody', location='@sun', epochs={'start': ephemerides_start_date, 'stop': ephemerides_end_date, 'step': ephemerides_step}) - if param['OUT_FORM'] == 'XV': + if (param['OUT_FORM'] == 'XV' or param['OUT_FORM'] == 'XVEL'): p1.append(pldata[key].vectors()['x'][0] * DCONV) p2.append(pldata[key].vectors()['y'][0] * DCONV) p3.append(pldata[key].vectors()['z'][0] * DCONV) @@ -174,36 +217,52 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): p6.append(pldata[key].vectors()['vz'][0] * VCONV) p7.append(pldata[key].elements()['a'][0] * DCONV) p8.append(pldata[key].elements()['e'][0]) - p9.append(pldata[key].elements()['incl'][0] * np.pi / 180.0) - p10.append(pldata[key].elements()['Omega'][0] * np.pi / 180.0) - p11.append(pldata[key].elements()['w'][0] * np.pi / 180.0) - p12.append(pldata[key].elements()['M'][0] * np.pi / 180.0) + p9.append(pldata[key].elements()['incl'][0]) + p10.append(pldata[key].elements()['Omega'][0]) + p11.append(pldata[key].elements()['w'][0]) + p12.append(pldata[key].elements()['M'][0]) elif param['OUT_FORM'] == 'EL': p1.append(pldata[key].elements()['a'][0] * DCONV) p2.append(pldata[key].elements()['e'][0]) - p3.append(pldata[key].elements()['incl'][0] * np.pi / 180.0) - p4.append(pldata[key].elements()['Omega'][0] * np.pi / 180.0) - p5.append(pldata[key].elements()['w'][0] * np.pi / 180.0) - p6.append(pldata[key].elements()['M'][0] * np.pi / 180.0) + p3.append(pldata[key].elements()['incl'][0]) + p4.append(pldata[key].elements()['Omega'][0]) + p5.append(pldata[key].elements()['w'][0]) + p6.append(pldata[key].elements()['M'][0]) p7.append(pldata[key].vectors()['x'][0] * DCONV) p8.append(pldata[key].vectors()['y'][0] * DCONV) p9.append(pldata[key].vectors()['z'][0] * DCONV) p10.append(pldata[key].vectors()['vx'][0] * VCONV) p11.append(pldata[key].vectors()['vy'][0] * VCONV) p12.append(pldata[key].vectors()['vz'][0] * VCONV) + pvec = np.vstack([p1, p2, p3, p4, p5, p6, p7, p8, p9, p10, p11, p12]) + if ispl: Rpl.append(planetradius[key] * DCONV) GMpl.append(GMcb[0] / MSun_over_Mpl[key]) + pvec = np.vstack([pvec, GMpl, Rpl]) + # Generate planet value vectors if (param['RHILL_PRESENT'] == 'YES'): - Rhill.append(pldata[key].elements()['a'][0] * DCONV * (3 * MSun_over_Mpl[key]) ** (-THIRDLONG)) - pvec = np.vstack([p1, p2, p3, p4, p5, p6, GMpl, Rpl, Rhill, p7, p8, p9, p10, p11, p12]) - else: - pvec = np.vstack([p1, p2, p3, p4, p5, p6, GMpl, Rpl, p7, p8, p9, p10, p11, p12]) + rhill.append(pldata[key].elements()['a'][0] * DCONV * (3 * MSun_over_Mpl[key]) ** (-THIRDLONG)) + pvec = np.vstack([pvec, rhill]) + if (param['ROTATION'] == 'YES'): + RA = pldata[key].ephemerides()['NPole_RA'][0] + DEC = pldata[key].ephemerides()['NPole_DEC'][0] + + rotpole = SkyCoord(ra=RA * u.degree, dec=DEC * u.degree) + rotrate = planetrot[key] * param['TU2S'] + rot = rotpole.cartesian * rotrate + Ip = np.array([0.0, 0.0, planetIpz[key]]) + Ip1.append(Ip[0]) + Ip2.append(Ip[1]) + Ip3.append(Ip[2]) + rotx.append(rot.x) + roty.append(rot.y) + rotz.append(rot.z) + pvec = np.vstack([pvec, Ip1, Ip2, Ip3, rotx, roty, rotz]) else: - pvec = np.vstack([p1, p2, p3, p4, p5, p6, p7, p8, p9, p10, p11, p12]) plab = tlab.copy() - + if idval is None: plid = np.array([planetid[key]], dtype=int) else: @@ -212,7 +271,60 @@ def solar_system_horizons(plname, idval, param, ephemerides_start_date, ds): # Prepare frames by adding an extra axis for the time coordinate plframe = np.expand_dims(pvec.T, axis=0) plxr = xr.DataArray(plframe, dims=dims, coords={'time': t, 'id': plid, 'vec': plab}) + plxr = plxr.assign_coords(name=('id', [plname])) plds = plxr.to_dataset(dim='vec') ds = xr.combine_by_coords([ds, plds]) + return ds + +def vec2xr(param, idvals, namevals, v1, v2, v3, v4, v5, v6, GMpl=None, Rpl=None, rhill=None, Ip1=None, Ip2=None, Ip3=None, rotx=None, roty=None, rotz=None, t=0.0): + + if param['ROTATION'] == 'YES': + if Ip1 is None: + Ip1 = np.full_like(v1, 0.4) + if Ip2 is None: + Ip2 = np.full_like(v1, 0.4) + if Ip3 is None: + Ip3 = np.full_like(v1, 0.4) + if rotx is None: + rotx = np.full_like(v1, 0.0) + if roty is None: + roty = np.full_like(v1, 0.0) + if rotz is None: + rotz = np.full_like(v1, 0.0) + + dims = ['time', 'id', 'vec'] + if GMpl is not None: + ispl = True + else: + ispl = False + + if ispl and Rpl is None: + print("Massive bodies need a radius value.") + return None + if ispl and rhill is None and param['RHILL_PRESENT'] == 'YES': + print("rhill is required.") + return None + + # Be sure we use the correct input format + old_out_form = param['OUT_FORM'] + param['OUT_FORM'] = param['IN_FORM'] + clab, plab, tlab = swiftest.io.make_swiftest_labels(param) + param['OUT_FORM'] = old_out_form + vec = np.vstack([v1, v2, v3, v4, v5, v6]) + if ispl: + vec = np.vstack([vec, GMpl, Rpl]) + if param['RHILL_PRESENT'] == 'YES': + vec = np.vstack([vec, rhill]) + if param['ROTATION'] == 'YES': + vec = np.vstack([vec, Ip1, Ip2, Ip3, rotx, roty, rotz]) + bodyframe = np.expand_dims(vec.T, axis=0) + if ispl: + bodyxr = xr.DataArray(bodyframe, dims=dims, coords={'time': [t], 'id': idvals, 'vec': plab}) + else: + bodyxr = xr.DataArray(bodyframe, dims=dims, coords={'time': [t], 'id': idvals, 'vec': tlab}) + + bodyxr = bodyxr.assign_coords(name=('id', namevals)) + + ds = bodyxr.to_dataset(dim='vec') return ds \ No newline at end of file diff --git a/python/swiftest/swiftest/io.py b/python/swiftest/swiftest/io.py index 0492a05f8..da1c49f17 100644 --- a/python/swiftest/swiftest/io.py +++ b/python/swiftest/swiftest/io.py @@ -5,7 +5,7 @@ import sys import tempfile -newfeaturelist = ("FRAGMENTATION", "ROTATION", "TIDES", "ENERGY", "GR", "YARKOVSKY", "YORP") +newfeaturelist = ("FRAGMENTATION", "ROTATION", "TIDES", "ENERGY", "GR", "YARKOVSKY", "YORP", "IN_FORM") def real2float(realstr): """ @@ -285,8 +285,6 @@ def write_labeled_param(param, param_file_name): 'TP_IN', 'CB_IN', 'BIN_OUT', - 'ENC_OUT', - 'DISCARD_OUT', 'CHK_QMIN', 'CHK_RMIN', 'CHK_RMAX', @@ -303,7 +301,7 @@ def write_labeled_param(param, param_file_name): if val is not None: print(f"{key:<16} {val}", file=outfile) # Print the remaining key/value pairs in whatever order for key, val in ptmp.items(): - print(f"{key:<16} {val}", file=outfile) + if val != "": print(f"{key:<16} {val}", file=outfile) outfile.close() return @@ -326,7 +324,7 @@ def swifter_stream(f, param): plid : int array IDs of massive bodies pvec : float array - (npl,N) - vector of N quantities or each particle (6 of XV/EL + GMass, Radius, etc) + (npl,N) - vector of N quantities or each particle (6 of XV/EL + Gmass, radius, etc) plab : string list Labels for the pvec data ntp : int @@ -353,13 +351,13 @@ def swifter_stream(f, param): tvec = np.empty((6, ntp)) tpid = np.empty(ntp, dtype='int') if npl > 0: - Mpl = np.empty(npl) + GMpl = np.empty(npl) Rpl = np.empty(npl) for i in range(npl): # Read single-line pl frame for record = f.read_record(' 0: @@ -369,14 +367,14 @@ def swifter_stream(f, param): tvec[:, i] = record[1] tlab = [] - if param['OUT_FORM'] == 'XV': - tlab.append('px') - tlab.append('py') - tlab.append('pz') - tlab.append('vx') - tlab.append('vy') - tlab.append('vz') - elif param['OUT_FORM'] == 'EL': + if param['OUT_FORM'] == 'XV' or param['OUT_FORM'] == 'XVEL': + tlab.append('xhx') + tlab.append('xhy') + tlab.append('xhz') + tlab.append('vhx') + tlab.append('vhy') + tlab.append('vhz') + if param['OUT_FORM'] == 'EL' or param['OUT_FORM'] == 'XVEL': tlab.append('a') tlab.append('e') tlab.append('inc') @@ -384,9 +382,9 @@ def swifter_stream(f, param): tlab.append('omega') tlab.append('capm') plab = tlab.copy() - plab.append('GMass') - plab.append('Radius') - pvec = np.vstack([pvec, Mpl, Rpl]) + plab.append('Gmass') + plab.append('radius') + pvec = np.vstack([pvec, GMpl, Rpl]) yield t, npl, plid, pvec.T, plab, \ ntp, tpid, tvec.T, tlab @@ -394,14 +392,15 @@ def swifter_stream(f, param): def make_swiftest_labels(param): tlab = [] - if param['OUT_FORM'] == 'XV': - tlab.append('px') - tlab.append('py') - tlab.append('pz') - tlab.append('vx') - tlab.append('vy') - tlab.append('vz') - elif param['OUT_FORM'] == 'EL': + if param['OUT_FORM'] == 'XV' or param['OUT_FORM'] == 'XVEL': + tlab.append('xhx') + tlab.append('xhy') + tlab.append('xhz') + tlab.append('vhx') + tlab.append('vhy') + tlab.append('vhz') + + if param['OUT_FORM'] == 'EL' or param['OUT_FORM'] == 'XVEL': tlab.append('a') tlab.append('e') tlab.append('inc') @@ -409,24 +408,24 @@ def make_swiftest_labels(param): tlab.append('omega') tlab.append('capm') plab = tlab.copy() - plab.append('GMass') - plab.append('Radius') + plab.append('Gmass') + plab.append('radius') if param['RHILL_PRESENT'] == 'YES': - plab.append('Rhill') - clab = ['GMass', 'Radius', 'J_2', 'J_4'] + plab.append('rhill') + clab = ['Gmass', 'radius', 'J_2', 'J_4'] if param['ROTATION'] == 'YES': - clab.append('Ip_x') - clab.append('Ip_y') - clab.append('Ip_z') - clab.append('rot_x') - clab.append('rot_y') - clab.append('rot_z') - plab.append('Ip_x') - plab.append('Ip_y') - plab.append('Ip_z') - plab.append('rot_x') - plab.append('rot_y') - plab.append('rot_z') + clab.append('Ip1') + clab.append('Ip2') + clab.append('Ip3') + clab.append('rotx') + clab.append('roty') + clab.append('rotz') + plab.append('Ip1') + plab.append('Ip2') + plab.append('Ip3') + plab.append('rotx') + plab.append('roty') + plab.append('rotz') if param['TIDES'] == 'YES': clab.append('k2') clab.append('Q') @@ -451,13 +450,13 @@ def swiftest_stream(f, param): cbid : int array ID of central body (always returns 0) cvec : float array - (npl,1) - vector of quantities for the massive body (GMass, Radius, J2, J4, etc) + (npl,1) - vector of quantities for the massive body (Gmass, radius, J2, J4, etc) npl : int Number of massive bodies plid : int array IDs of massive bodies pvec : float array - (npl,N) - vector of N quantities or each particle (6 of XV/EL + GMass, Radius, etc) + (npl,N) - vector of N quantities or each particle (6 of XV/EL + Gmass, radius, etc) plab : string list Labels for the pvec data ntp : int @@ -469,6 +468,7 @@ def swiftest_stream(f, param): tlab : string list Labels for the tvec data """ + NAMELEN = 32 while True: # Loop until you read the end of file try: # Read multi-line header @@ -479,6 +479,9 @@ def swiftest_stream(f, param): ntp = f.read_ints() iout_form = f.read_reals('c') cbid = f.read_ints() + dtstr = f'a{NAMELEN}' + cbnames = f.read_record(dtstr) + cbnames = [np.char.strip(str(cbnames[0], encoding='utf-8'))] Mcb = f.read_reals(np.float64) Rcb = f.read_reals(np.float64) J2cb = f.read_reals(np.float64) @@ -495,15 +498,27 @@ def swiftest_stream(f, param): Qcb = f.read_reals(np.float64) if npl[0] > 0: plid = f.read_ints() + dtstr = f'({npl[0]},)a{NAMELEN}' + names = f.read_record(np.dtype(dtstr)) + plnames = [] + for i in range(npl[0]): + plnames.append(np.char.strip(str(names[i], encoding='utf-8'))) p1 = f.read_reals(np.float64) p2 = f.read_reals(np.float64) p3 = f.read_reals(np.float64) p4 = f.read_reals(np.float64) p5 = f.read_reals(np.float64) p6 = f.read_reals(np.float64) - Mpl = f.read_reals(np.float64) + if param['OUT_FORM'] == 'XVEL': + p7 = f.read_reals(np.float64) + p8 = f.read_reals(np.float64) + p9 = f.read_reals(np.float64) + p10 = f.read_reals(np.float64) + p11 = f.read_reals(np.float64) + p12 = f.read_reals(np.float64) + GMpl = f.read_reals(np.float64) if param['RHILL_PRESENT'] == 'YES': - Rhill = f.read_reals(np.float64) + rhill = f.read_reals(np.float64) Rpl = f.read_reals(np.float64) if param['ROTATION'] == 'YES': Ipplx = f.read_reals(np.float64) @@ -517,29 +532,54 @@ def swiftest_stream(f, param): Qpl = f.read_reals(np.float64) if ntp[0] > 0: tpid = f.read_ints() + dtstr = f'({ntp[0]},)a{NAMELEN}' + names = f.read_record(np.dtype(dtstr)) + tpnames = [] + for i in range(npl[0]): + tpnames.append(np.char.strip(str(names[i], encoding='utf-8'))) t1 = f.read_reals(np.float64) t2 = f.read_reals(np.float64) t3 = f.read_reals(np.float64) t4 = f.read_reals(np.float64) t5 = f.read_reals(np.float64) t6 = f.read_reals(np.float64) + if param['OUT_FORM'] == 'XVEL': + t7 = f.read_reals(np.float64) + t8 = f.read_reals(np.float64) + t9 = f.read_reals(np.float64) + t10 = f.read_reals(np.float64) + t11 = f.read_reals(np.float64) + t12 = f.read_reals(np.float64) clab, plab, tlab = make_swiftest_labels(param) - + if npl > 0: - pvec = np.vstack([p1, p2, p3, p4, p5, p6, Mpl, Rpl]) + pvec = np.vstack([p1, p2, p3, p4, p5, p6]) + if param['OUT_FORM'] == 'XVEL': + pvec = np.vstack([pvec, p7, p8, p9, p10, p11, p12]) + pvec = np.vstack([pvec, GMpl, Rpl]) else: - pvec = np.empty((8, 0)) + if param['OUT_FORM'] == 'XVEL': + pvec = np.empty((14, 0)) + else: + pvec = np.empty((8, 0)) plid = np.empty(0) + plnames = np.empty(0) if ntp > 0: tvec = np.vstack([t1, t2, t3, t4, t5, t6]) + if param['OUT_FORM'] == 'XVEL': + tvec = np.vstack([tvec, t7, t8, t9, t10, t11, t12]) else: - tvec = np.empty((6, 0)) + if param['OUT_FORM'] == 'XVEL': + tvec = np.empty((12, 0)) + else: + tvec = np.empty((6, 0)) tpid = np.empty(0) + tpnames = np.empty(0) cvec = np.array([Mcb, Rcb, J2cb, J4cb]) if param['RHILL_PRESENT'] == 'YES': if npl > 0: - pvec = np.vstack([pvec, Rhill]) + pvec = np.vstack([pvec, rhill]) if param['ROTATION'] == 'YES': cvec = np.vstack([cvec, Ipcbx, Ipcby, Ipcbz, rotcbx, rotcby, rotcbz]) if npl > 0: @@ -548,9 +588,9 @@ def swiftest_stream(f, param): cvec = np.vstack([cvec, k2cb, Qcb]) if npl > 0: pvec = np.vstack([pvec, k2pl, Qpl]) - yield t, cbid, cvec.T, clab, \ - npl, plid, pvec.T, plab, \ - ntp, tpid, tvec.T, tlab + yield t, cbid, cbnames, cvec.T, clab, \ + npl, plid, plnames, pvec.T, plab, \ + ntp, tpid, tpnames, tvec.T, tlab def swifter2xr(param): @@ -609,47 +649,86 @@ def swiftest2xr(param): ------- xarray dataset """ + if ((param['OUT_TYPE'] == 'REAL8') or (param['OUT_TYPE'] == 'REAL4')): + dims = ['time', 'id', 'vec'] + cb = [] + pl = [] + tp = [] + cbn = None + try: + with FortranFile(param['BIN_OUT'], 'r') as f: + for t, cbid, cbnames, cvec, clab, \ + npl, plid, plnames, pvec, plab, \ + ntp, tpid, tpnames, tvec, tlab in swiftest_stream(f, param): + # Prepare frames by adding an extra axis for the time coordinate + cbframe = np.expand_dims(cvec, axis=0) + plframe = np.expand_dims(pvec, axis=0) + tpframe = np.expand_dims(tvec, axis=0) + + + # Create xarray DataArrays out of each body type + cbxr = xr.DataArray(cbframe, dims=dims, coords={'time': t, 'id': cbid, 'vec': clab}) + cbxr = cbxr.assign_coords(name=("id", cbnames)) + plxr = xr.DataArray(plframe, dims=dims, coords={'time': t, 'id': plid, 'vec': plab}) + plxr = plxr.assign_coords(name=("id", plnames)) + tpxr = xr.DataArray(tpframe, dims=dims, coords={'time': t, 'id': tpid, 'vec': tlab}) + tpxr = tpxr.assign_coords(name=("id", tpnames)) + + cb.append(cbxr) + pl.append(plxr) + tp.append(tpxr) + + sys.stdout.write('\r' + f"Reading in time {t[0]:.3e}") + sys.stdout.flush() + except IOError: + print(f"Error encountered reading in {param['BIN_OUT']}") + + cbda = xr.concat(cb, dim='time') + plda = xr.concat(pl, dim='time') + tpda = xr.concat(tp, dim='time') - dims = ['time', 'id', 'vec'] - cb = [] - pl = [] - tp = [] - try: - with FortranFile(param['BIN_OUT'], 'r') as f: - for t, cbid, cvec, clab, \ - npl, plid, pvec, plab, \ - ntp, tpid, tvec, tlab in swiftest_stream(f, param): - # Prepare frames by adding an extra axis for the time coordinate - cbframe = np.expand_dims(cvec, axis=0) - plframe = np.expand_dims(pvec, axis=0) - tpframe = np.expand_dims(tvec, axis=0) - - # Create xarray DataArrays out of each body type - cbxr = xr.DataArray(cbframe, dims=dims, coords={'time': t, 'id': cbid, 'vec': clab}) - plxr = xr.DataArray(plframe, dims=dims, coords={'time': t, 'id': plid, 'vec': plab}) - tpxr = xr.DataArray(tpframe, dims=dims, coords={'time': t, 'id': tpid, 'vec': tlab}) - - cb.append(cbxr) - pl.append(plxr) - tp.append(tpxr) - sys.stdout.write('\r' + f"Reading in time {t[0]:.3e}") - sys.stdout.flush() - except IOError: - print(f"Error encountered reading in {param['BIN_OUT']}") + cbds = cbda.to_dataset(dim='vec') + plds = plda.to_dataset(dim='vec') + tpds = tpda.to_dataset(dim='vec') + print('\nCreating Dataset') + ds = xr.combine_by_coords([cbds, plds, tpds]) - cbda = xr.concat(cb, dim='time') - plda = xr.concat(pl, dim='time') - tpda = xr.concat(tp, dim='time') - - cbds = cbda.to_dataset(dim='vec') - plds = plda.to_dataset(dim='vec') - tpds = tpda.to_dataset(dim='vec') - print('\nCreating Dataset') - ds = xr.combine_by_coords([cbds, plds, tpds]) + elif ((param['OUT_TYPE'] == 'NETCDF_DOUBLE') or (param['OUT_TYPE'] == 'NETCDF_FLOAT')): + print('\nCreating Dataset') + ds = xr.open_dataset(param['BIN_OUT']) + ds = clean_string_values(param, ds) + else: + print(f"Error encountered. OUT_TYPE {param['OUT_TYPE']} not recognized.") + return None print(f"Successfully converted {ds.sizes['time']} output frames.") - if param['PARTICLE_OUT'] != "": - ds = swiftest_particle_2xr(ds, param) - + + return ds + +def xstrip(a): + func = lambda x: np.char.strip(x) + return xr.apply_ufunc(func, a.str.decode(encoding='utf-8')) + +def clean_string_values(param, ds): + """ + Cleans up the string values in the DataSet that have artifacts as a result of coming from NetCDF Fortran + + Parameters + ---------- + param : dict + ds : xarray dataset + + Returns + ------- + ds : xarray dataset with the strings cleaned up + """ + if 'name' in ds: + ds['name'] = xstrip(ds['name']) + if 'particle_type' in ds: + ds['particle_type'] = xstrip(ds['particle_type']) + if 'status' in ds: + ds['status'] = xstrip(ds['status']) + if 'origin_type' in ds: + ds['origin_type'] = xstrip(ds['origin_type']) return ds @@ -685,9 +764,9 @@ def swiftest_particle_stream(f): yield plid, origin_type, origin_vec -def swiftest_particle_2xr(ds, param): +def swiftest_particle_2xr(param): """Reads in the Swiftest SyMBA-generated PARTICLE_OUT and converts it to an xarray Dataset""" - veclab = ['time_origin', 'px_origin', 'py_origin', 'pz_origin', 'vx_origin', 'vy_origin', 'vz_origin'] + veclab = ['time_origin', 'xhx_origin', 'py_origin', 'pz_origin', 'vhx_origin', 'vhy_origin', 'vhz_origin'] id_list = [] origin_type_list = [] origin_vec_list = [] @@ -711,9 +790,7 @@ def swiftest_particle_2xr(ds, param): infoxr = vecda.to_dataset(dim='vec') infoxr['origin_type'] = typeda - print('\nAdding particle info to Dataset') - ds = xr.merge([ds, infoxr]) - return ds + return infoxr def swiftest_xr2infile(ds, param, framenum=-1): @@ -736,23 +813,34 @@ def swiftest_xr2infile(ds, param, framenum=-1): frame = ds.isel(time=framenum) cb = frame.where(frame.id == 0, drop=True) pl = frame.where(frame.id > 0, drop=True) - pl = pl.where(np.invert(np.isnan(pl['GMass'])), drop=True).drop_vars(['J_2', 'J_4']) - tp = frame.where(np.isnan(frame['GMass']), drop=True).drop_vars(['GMass', 'Radius', 'J_2', 'J_4']) + pl = pl.where(np.invert(np.isnan(pl['Gmass'])), drop=True).drop_vars(['J_2', 'J_4']) + tp = frame.where(np.isnan(frame['Gmass']), drop=True).drop_vars(['Gmass', 'radius', 'J_2', 'J_4']) - GMSun = np.double(cb['GMass']) - RSun = np.double(cb['Radius']) + GMSun = np.double(cb['Gmass']) + RSun = np.double(cb['radius']) J2 = np.double(cb['J_2']) J4 = np.double(cb['J_4']) + cbname = cb['name'].values[0] + if param['ROTATION'] == 'YES': + Ip1cb = np.double(cb['Ip1']) + Ip2cb = np.double(cb['Ip2']) + Ip3cb = np.double(cb['Ip3']) + rotxcb = np.double(cb['rotx']) + rotycb = np.double(cb['roty']) + rotzcb = np.double(cb['rotz']) cbid = int(0) if param['IN_TYPE'] == 'ASCII': # Swiftest Central body file cbfile = open(param['CB_IN'], 'w') - print(0, file=cbfile) + print(cbname, file=cbfile) print(GMSun, file=cbfile) print(RSun, file=cbfile) print(J2, file=cbfile) print(J4, file=cbfile) + if param['ROTATION'] == 'YES': + print(Ip1cb, Ip2cb, Ip3cb, file=cbfile) + print(rotxcb, rotycb, rotzcb, file=cbfile) cbfile.close() plfile = open(param['PL_IN'], 'w') @@ -760,12 +848,21 @@ def swiftest_xr2infile(ds, param, framenum=-1): for i in pl.id: pli = pl.sel(id=i) if param['RHILL_PRESENT'] == 'YES': - print(i.values, pli['GMass'].values, pli['Rhill'].values, file=plfile) + print(pli['name'].values, pli['Gmass'].values, pli['rhill'].values, file=plfile) + else: + print(pli['name'].values, pli['Gmass'].values, file=plfile) + print(pli['radius'].values, file=plfile) + if param['IN_FORM'] == 'XV': + print(pli['xhx'].values, pli['xhy'].values, pli['xhz'].values, file=plfile) + print(pli['vhx'].values, pli['vhy'].values, pli['vhz'].values, file=plfile) + elif param['IN_FORM'] == 'EL': + print(pli['a'].values, pli['e'].values, pli['inc'].values, file=plfile) + print(pli['capom'].values, pli['omega'].values, pli['capm'].values, file=plfile) else: - print(i.values, pli['GMass'].values, file=plfile) - print(pli['Radius'].values, file=plfile) - print(pli['px'].values, pli['py'].values, pli['pz'].values, file=plfile) - print(pli['vx'].values, pli['vy'].values, pli['vz'].values, file=plfile) + print(f"{param['IN_FORM']} is not a valid input format type.") + if param['ROTATION'] == 'YES': + print(pli['Ip1'].values, pli['Ip2'].values, pli['Ip3'].values, file=plfile) + print(pli['rotx'].values, pli['roty'].values, pli['rotz'].values, file=plfile) plfile.close() # TP file @@ -773,9 +870,15 @@ def swiftest_xr2infile(ds, param, framenum=-1): print(tp.id.count().values, file=tpfile) for i in tp.id: tpi = tp.sel(id=i) - print(i.values, file=tpfile) - print(tpi['px'].values, tpi['py'].values, tpi['pz'].values, file=tpfile) - print(tpi['vx'].values, tpi['vy'].values, tpi['vz'].values, file=tpfile) + print(tpi['name'].values, file=tpfile) + if param['IN_FORM'] == 'XV': + print(tpi['xhx'].values, tpi['xhy'].values, tpi['xhz'].values, file=tpfile) + print(tpi['vhx'].values, tpi['vhy'].values, tpi['vhz'].values, file=tpfile) + elif param['IN_FORM'] == 'EL': + print(tpi['a'].values, tpi['e'].values, tpi['inc'].values, file=tpfile) + print(tpi['capom'].values, tpi['omega'].values, tpi['capm'].values, file=tpfile) + else: + print(f"{param['IN_FORM']} is not a valid input format type.") tpfile.close() elif param['IN_TYPE'] == 'REAL8': # Now make Swiftest files @@ -785,51 +888,85 @@ def swiftest_xr2infile(ds, param, framenum=-1): cbfile.write_record(np.double(RSun)) cbfile.write_record(np.double(J2)) cbfile.write_record(np.double(J4)) + if param['ROTATION'] == 'YES': + cbfile.write_record(np.double(Ip1cb)) + cbfile.write_record(np.double(Ip2cb)) + cbfile.write_record(np.double(Ip3cb)) + cbfile.write_record(np.double(rotxcb)) + cbfile.write_record(np.double(rotycb)) + cbfile.write_record(np.double(rotzcb)) + cbfile.close() plfile = FortranFile(param['PL_IN'], 'w') npl = pl.id.count().values plid = pl.id.values - px = pl['px'].values - py = pl['py'].values - pz = pl['pz'].values - vx = pl['vx'].values - vy = pl['vy'].values - vz = pl['vz'].values - Gmass = pl['GMass'].values - radius = pl['Radius'].values + if param['IN_FORM'] == 'XV': + v1 = pl['xhx'].values + v2 = pl['xhy'].values + v3 = pl['xhz'].values + v4 = pl['vhx'].values + v5 = pl['vhy'].values + v6 = pl['vhz'].values + elif param['IN_FORM'] == 'EL': + v1 = pl['a'].values + v2 = pl['e'].values + v3 = pl['inc'].values + v4 = pl['capom'].values + v5 = pl['omega'].values + v6 = pl['capm'].values + else: + print(f"{param['IN_FORM']} is not a valid input format type.") + Gmass = pl['Gmass'].values + radius = pl['radius'].values plfile.write_record(npl) plfile.write_record(plid) - plfile.write_record(px) - plfile.write_record(py) - plfile.write_record(pz) - plfile.write_record(vx) - plfile.write_record(vy) - plfile.write_record(vz) + plfile.write_record(v1) + plfile.write_record(v2) + plfile.write_record(v3) + plfile.write_record(v4) + plfile.write_record(v5) + plfile.write_record(v6) plfile.write_record(Gmass) if param['RHILL_PRESENT'] == 'YES': - rhill = pl['Rhill'].values - plfile.write_record(rhill) + plfile.write_record(pl['rhill'].values) plfile.write_record(radius) + if param['ROTATION'] == 'YES': + plfile.write_record(pl['Ip1'].values) + plfile.write_record(pl['Ip2'].values) + plfile.write_record(pl['Ip3'].values) + plfile.write_record(pl['rotx'].values) + plfile.write_record(pl['roty'].values) + plfile.write_record(pl['rotz'].values) plfile.close() tpfile = FortranFile(param['TP_IN'], 'w') ntp = tp.id.count().values tpid = tp.id.values - px = tp['px'].values - py = tp['py'].values - pz = tp['pz'].values - vx = tp['vx'].values - vy = tp['vy'].values - vz = tp['vz'].values + if param['IN_FORM'] == 'XV': + v1 = tp['xhx'].values + v2 = tp['xhy'].values + v3 = tp['xhz'].values + v4 = tp['vhx'].values + v5 = tp['vhy'].values + v6 = tp['vhz'].values + elif param['IN_FORM'] == 'EL': + v1 = tp['a'].values + v2 = tp['e'].values + v3 = tp['inc'].values + v4 = tp['capom'].values + v5 = tp['omega'].values + v6 = tp['capm'].values + else: + print(f"{param['IN_FORM']} is not a valid input format type.") tpfile.write_record(ntp) tpfile.write_record(tpid) - tpfile.write_record(px) - tpfile.write_record(py) - tpfile.write_record(pz) - tpfile.write_record(vx) - tpfile.write_record(vy) - tpfile.write_record(vz) + tpfile.write_record(v1) + tpfile.write_record(v2) + tpfile.write_record(v3) + tpfile.write_record(v4) + tpfile.write_record(v5) + tpfile.write_record(v6) else: print(f"{param['IN_TYPE']} is an unknown file type") @@ -854,11 +991,11 @@ def swifter_xr2infile(ds, param, framenum=-1): frame = ds.isel(time=framenum) cb = frame.where(frame.id == 0, drop=True) pl = frame.where(frame.id > 0, drop=True) - pl = pl.where(np.invert(np.isnan(pl['GMass'])), drop=True).drop_vars(['J_2', 'J_4']) - tp = frame.where(np.isnan(frame['GMass']), drop=True).drop_vars(['GMass', 'Radius', 'J_2', 'J_4']) + pl = pl.where(np.invert(np.isnan(pl['Gmass'])), drop=True).drop_vars(['J_2', 'J_4']) + tp = frame.where(np.isnan(frame['Gmass']), drop=True).drop_vars(['Gmass', 'radius', 'J_2', 'J_4']) - GMSun = np.double(cb['GMass']) - RSun = np.double(cb['Radius']) + GMSun = np.double(cb['Gmass']) + RSun = np.double(cb['radius']) param['J2'] = np.double(cb['J_2']) param['J4'] = np.double(cb['J_4']) @@ -866,19 +1003,19 @@ def swifter_xr2infile(ds, param, framenum=-1): # Swiftest Central body file plfile = open(param['PL_IN'], 'w') print(pl.id.count().values + 1, file=plfile) - print(cb.id.values[0], cb['GMass'].values[0], file=plfile) + print(cb.id.values[0], GMSun, file=plfile) print('0.0 0.0 0.0', file=plfile) print('0.0 0.0 0.0', file=plfile) for i in pl.id: pli = pl.sel(id=i) if param['RHILL_PRESENT'] == "YES": - print(i.values, pli['GMass'].values, pli['Rhill'].values, file=plfile) + print(i.values, pli['Gmass'].values, pli['rhill'].values, file=plfile) else: - print(i.values, pli['GMass'].values, file=plfile) + print(i.values, pli['Gmass'].values, file=plfile) if param['CHK_CLOSE'] == "YES": - print(pli['Radius'].values, file=plfile) - print(pli['px'].values, pli['py'].values, pli['pz'].values, file=plfile) - print(pli['vx'].values, pli['vy'].values, pli['vz'].values, file=plfile) + print(pli['radius'].values, file=plfile) + print(pli['xhx'].values, pli['xhy'].values, pli['xhz'].values, file=plfile) + print(pli['vhx'].values, pli['vhy'].values, pli['vhz'].values, file=plfile) plfile.close() # TP file @@ -887,8 +1024,8 @@ def swifter_xr2infile(ds, param, framenum=-1): for i in tp.id: tpi = tp.sel(id=i) print(i.values, file=tpfile) - print(tpi['px'].values, tpi['py'].values, tpi['pz'].values, file=tpfile) - print(tpi['vx'].values, tpi['vy'].values, tpi['vz'].values, file=tpfile) + print(tpi['xhx'].values, tpi['xhy'].values, tpi['xhz'].values, file=tpfile) + print(tpi['vhx'].values, tpi['vhy'].values, tpi['vhz'].values, file=tpfile) tpfile.close() else: # Now make Swiftest files @@ -1024,14 +1161,14 @@ def swift2swifter(swift_param, plname="", tpname="", conversion_questions={}): i_list = [i for i in line.split(" ") if i.strip()] GMpl = real2float(i_list[0]) if isSyMBA: - Rhill = real2float(i_list[1]) + rhill = real2float(i_list[1]) if swift_param['LCLOSE'] == "T": plrad = real2float(i_list[2]) else: if swift_param['LCLOSE'] == "T": plrad = real2float(i_list[1]) if swifter_param['RHILL_PRESENT'] == 'YES': - print(n + 1, GMpl, Rhill, file=plnew) + print(n + 1, GMpl, rhill, file=plnew) else: print(n + 1, GMpl, file=plnew) if swifter_param['CHK_CLOSE'] == 'YES': @@ -1044,10 +1181,10 @@ def swift2swifter(swift_param, plname="", tpname="", conversion_questions={}): print(xh, yh, zh, file=plnew) line = plold.readline() i_list = [i for i in line.split(" ") if i.strip()] - vx = real2float(i_list[0]) - vy = real2float(i_list[1]) - vz = real2float(i_list[2]) - print(vx, vy, vz, file=plnew) + vhx = real2float(i_list[0]) + vhy = real2float(i_list[1]) + vhz = real2float(i_list[2]) + print(vhx, vhy, vhz, file=plnew) plnew.close() plold.close() except IOError: @@ -1083,10 +1220,10 @@ def swift2swifter(swift_param, plname="", tpname="", conversion_questions={}): print(xh, yh, zh, file=tpnew) line = tpold.readline() i_list = [i for i in line.split(" ") if i.strip()] - vx = real2float(i_list[0]) - vy = real2float(i_list[1]) - vz = real2float(i_list[2]) - print(vx, vy, vz, file=tpnew) + vhx = real2float(i_list[0]) + vhy = real2float(i_list[1]) + vhz = real2float(i_list[2]) + print(vhx, vhy, vhz, file=tpnew) # Ignore STAT lines line = tpold.readline() line = tpold.readline() @@ -1134,8 +1271,8 @@ def swifter2swiftest(swifter_param, plname="", tpname="", cbname="", conversion_ idnum = int(i_list[0]) GMpl = real2float(i_list[1]) if swifter_param['RHILL_PRESENT'] == 'YES': - Rhill = real2float(i_list[2]) - print(idnum, GMpl, Rhill, file=plnew) + rhill = real2float(i_list[2]) + print(idnum, GMpl, rhill, file=plnew) else: print(idnum, GMpl, file=plnew) if swifter_param['CHK_CLOSE'] == 'YES': @@ -1151,10 +1288,10 @@ def swifter2swiftest(swifter_param, plname="", tpname="", cbname="", conversion_ print(xh, yh, zh, file=plnew) line = plold.readline() i_list = [i for i in line.split(" ") if i.strip()] - vx = real2float(i_list[0]) - vy = real2float(i_list[1]) - vz = real2float(i_list[2]) - print(vx, vy, vz, file=plnew) + vhx = real2float(i_list[0]) + vhy = real2float(i_list[1]) + vhz = real2float(i_list[2]) + print(vhx, vhy, vhz, file=plnew) plnew.close() plold.close() except IOError: @@ -1195,10 +1332,10 @@ def swifter2swiftest(swifter_param, plname="", tpname="", cbname="", conversion_ print(xh, yh, zh, file=tpnew) line = tpold.readline() i_list = [i for i in line.split(" ") if i.strip()] - vx = real2float(i_list[0]) - vy = real2float(i_list[1]) - vz = real2float(i_list[2]) - print(vx, vy, vz, file=tpnew) + vhx = real2float(i_list[0]) + vhy = real2float(i_list[1]) + vhz = real2float(i_list[2]) + print(vhx, vhy, vhz, file=tpnew) tpold.close() tpnew.close() @@ -1366,4 +1503,53 @@ def swiftest2swifter_param(swiftest_param, J2=0.0, J4=0.0): swifter_param['OUT_STAT'] = "UNKNOWN" swifter_param['! VERSION'] = "Swifter parameter file converted from Swiftest" - return swifter_param \ No newline at end of file + return swifter_param + + +def swifter2swift_param(swifter_param, J2=0.0, J4=0.0): + swift_param = { + '! VERSION': f"Swift parameter input file converted from Swifter", + 'T0': 0.0, + 'TSTOP': 0.0, + 'DT': 0.0, + 'DTOUT': 0.0, + 'DTDUMP': 0.0, + 'L1': "F", + 'L1': "F", + 'L2': "F", + 'L3': "F", + 'L4': "F", + 'L5': "T", + 'L6': "F", + 'RMIN': -1, + 'RMAX': -1, + 'RMAXU': -1, + 'QMIN': -1, + 'LCLOSE': "F", + 'BINARY_OUTPUTFILE': "bin.dat", + 'STATUS_FLAG_FOR_OPEN_STATEMENTS': "NEW", + } + + swift_param['T0'] = swifter_param['T0'] + swift_param['TSTOP'] = swifter_param['TSTOP'] + swift_param['DT'] = swifter_param['DT'] + # Convert the parameter file values + swift_param['DTOUT'] = swifter_param['ISTEP_OUT'] * swifter_param['DT'] + swift_param['DTDUMP'] = swifter_param['ISTEP_DUMP'] * swifter_param['DT'] + swift_param['BINARY_OUTPUTFILE'] = swifter_param['BIN_OUT'] + swift_param['STATUS_FLAG_FOR_OPEN_STATEMENTS'] = swifter_param['OUT_STAT'] + + if swifter_param['CHK_CLOSE'] == "YES": + swift_param['LCLOSE'] = "T" + else: + swift_param['LCLOSE'] = "F" + + swift_param['RMIN'] = swifter_param['CHK_RMIN'] + swift_param['RMAX'] = swifter_param['CHK_RMAX'] + swift_param['QMIN'] = swifter_param['CHK_QMIN'] + + if swift_param['RMIN'] > 0 or swift_param['RMAX'] > 0 or swift_param['QMIN'] > 0: + swift_param['L2'] = 'T' + + + return swift_param \ No newline at end of file diff --git a/python/swiftest/swiftest/simulation_class.py b/python/swiftest/swiftest/simulation_class.py index fc5075ab9..b2736c96d 100644 --- a/python/swiftest/swiftest/simulation_class.py +++ b/python/swiftest/swiftest/simulation_class.py @@ -4,6 +4,7 @@ from swiftest import constants from datetime import date import xarray as xr +import numpy as np class Simulation: """ @@ -20,18 +21,19 @@ def __init__(self, codename="Swiftest", param_file=""): 'TP_IN': "tp.in", 'CB_IN': "cb.in", 'IN_TYPE': "ASCII", + 'IN_FORM': "EL", 'ISTEP_OUT': "1", 'ISTEP_DUMP': "1", - 'BIN_OUT': "bin.dat", - 'OUT_TYPE': 'REAL8', - 'OUT_FORM': "EL", + 'BIN_OUT': "bin.nc", + 'OUT_TYPE': 'NETCDF_DOUBLE', + 'OUT_FORM': "XVEL", 'OUT_STAT': "REPLACE", - 'CHK_RMAX': "1000.0", - 'CHK_EJECT': "1000.0", - 'CHK_RMIN': constants.RSun / constants.AU2M, - 'CHK_QMIN': constants.RSun / constants.AU2M, + 'CHK_RMAX': "-1.0", + 'CHK_EJECT': "-1.0", + 'CHK_RMIN': "-1.0", + 'CHK_QMIN': "-1.0", 'CHK_QMIN_COORD': "HELIO", - 'CHK_QMIN_RANGE': f"{constants.RSun / constants.AU2M} 1000.0", + 'CHK_QMIN_RANGE': "-1.0 -1.0", 'ENC_OUT': "enc.dat", 'MU2KG': constants.MSun, 'TU2S': constants.JD2S, @@ -72,6 +74,37 @@ def add(self, plname, date=date.today().isoformat(), idval=None): return + def addp(self, idvals, namevals, t1, t2, t3, t4, t5, t6, GMpl=None, Rpl=None, rhill=None, Ip1=None, Ip2=None, Ip3=None, rotx=None, roty=None, rotz=None): + """ + Adds a body (test particle or massive body) to the internal DataSet given a set up 6 vectors (orbital elements + or cartesian state vectors, depending on the value of self.param). Input all angles in degress + + Parameters + ---------- + idvals : Integer array of body index values. + t1 : xh for param['IN_FORM'] == "XV"; a for param['IN_FORM'] == "EL" + t2 : yh for param['IN_FORM'] == "XV"; e for param['IN_FORM'] == "EL" + t3 : zh for param['IN_FORM'] == "XV"; inc for param['IN_FORM'] == "EL" + t4 : vhxh for param['IN_FORM'] == "XV"; capom for param['IN_FORM'] == "EL" + t5 : vhyh for param['IN_FORM'] == "XV"; omega for param['IN_FORM'] == "EL" + t6 : vhzh for param['IN_FORM'] == "XV"; capm for param['IN_FORM'] == "EL" + Gmass : Optional: Array of G*mass values if these are massive bodies + radius : Optional: Array radius values if these are massive bodies + rhill : Optional: Array rhill values if these are massive bodies + Ip1,y,z : Optional: Principal axes moments of inertia + rotx,y,z: Optional: Rotation rate vector components + Returns + ------- + self.ds : xarray dataset + """ + t = self.param['T0'] + + dsnew = init_cond.vec2xr(self.param, idvals, namevals, t1, t2, t3, t4, t5, t6, GMpl, Rpl, rhill, Ip1, Ip2, Ip3, rotx, roty, rotz, t) + if dsnew is not None: + self.ds = xr.combine_by_coords([self.ds, dsnew]) + return + + def read_param(self, param_file, codename="Swiftest"): if codename == "Swiftest": self.param = io.read_swiftest_param(param_file, self.param) diff --git a/python/swiftest/swiftest/tool.py b/python/swiftest/swiftest/tool.py index a96610bc2..efdc82a8b 100644 --- a/python/swiftest/swiftest/tool.py +++ b/python/swiftest/swiftest/tool.py @@ -8,10 +8,10 @@ """ def wrap_angle(angle): - while np.any(angle >= 2 * np.pi): - angle[angle >= 2 * np.pi] -= 2 * np.pi + while np.any(angle >= 360.0 ): + angle[angle >= 360.0] -= 360.0 while np.any(angle < 0.0): - angle[angle < 0.0] += 2 * np.pi + angle[angle < 0.0] += 360.0 return angle def follow_swift(ds, ifol=None, nskp=None): @@ -38,11 +38,11 @@ def follow_swift(ds, ifol=None, nskp=None): ifol = int(intxt) print(f"Following particle {ifol}") if ifol < 0: # Negative numbers are planets - fol = ds.where(np.invert(np.isnan(ds['GMass'])), drop=True) + fol = ds.where(np.invert(np.isnan(ds['Gmass'])), drop=True) fol = fol.where(np.invert(np.isnan(fol['a'])), drop=True) # Remove times where this body doesn't exist (but this also gets rid of the central body) fol = fol.isel(id = -ifol - 2) # Take 1 off for 0-indexed arrays in Python, and take 1 more off because the central body is gone elif ifol > 0: # Positive numbers are test particles - fol = ds.where(np.isnan(ds['GMass']), drop=True).drop_vars(['GMass', 'Radius']) + fol = ds.where(np.isnan(ds['Gmass']), drop=True).drop_vars(['Gmass', 'radius']) fol = fol.where(np.invert(np.isnan(fol['a'])), drop=True) fol = fol.isel(id = ifol - 1) # Take 1 off for 0-indexed arrays in Python @@ -50,15 +50,9 @@ def follow_swift(ds, ifol=None, nskp=None): intxt = input('Input the print frequency\n') nskp = int(intxt) - dr = 180.0 / np.pi fol['obar'] = fol['capom'] + fol['omega'] fol['obar'] = fol['obar'].fillna(0) fol['obar'] = wrap_angle(fol['obar']) - fol['obar'] = fol['obar'] * dr - fol['inc'] = fol['inc'] * dr - fol['capom'] = fol['capom'] * dr - fol['omega'] = fol['omega'] * dr - fol['capm'] = fol['capm'] * dr fol['peri'] = fol['a'] * (1.0 - fol['e']) fol['apo'] = fol['a'] * (1.0 + fol['e']) diff --git a/src/discard/discard.f90 b/src/discard/discard.f90 index 9c8044c61..2ee3dafec 100644 --- a/src/discard/discard.f90 +++ b/src/discard/discard.f90 @@ -31,7 +31,7 @@ module subroutine discard_system(self, param) end if if (lpl_discards .or. ltp_discards) call system%write_discard(param) - if (lpl_discards .and. param%lenergy) call self%conservation_report(param, lterminal=.true.) + if (lpl_discards .and. param%lenergy) call self%conservation_report(param, lterminal=.false.) if (lpl_check) call pl_discards%setup(0,param) if (ltp_check) call tp_discards%setup(0,param) @@ -53,7 +53,7 @@ module subroutine discard_pl(self, system, param) class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameter if (self%nbody == 0) return - self%ldiscard(:) = .false. + self%ldiscard(1:self%nbody) = .false. return end subroutine discard_pl @@ -73,9 +73,12 @@ module subroutine discard_tp(self, system, param) class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameter ! Internals logical, dimension(:), allocatable :: ldiscard + integer(I4B) :: npl, ntp - associate(tp => self, ntp => self%nbody, cb => system%cb, pl => system%pl, npl => system%pl%nbody) + associate(tp => self, cb => system%cb, pl => system%pl) if ((ntp == 0) .or. (npl ==0)) return + ntp = tp%nbody + npl = pl%nbody if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or. & (param%rmaxu >= 0.0_DP) .or. ((param%qmin >= 0.0_DP) .and. (param%qmin_coord == "BARY"))) then @@ -86,9 +89,9 @@ module subroutine discard_tp(self, system, param) if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or. (param%rmaxu >= 0.0_DP)) call discard_cb_tp(tp, system, param) if (param%qmin >= 0.0_DP) call discard_peri_tp(tp, system, param) if (param%lclose) call discard_pl_tp(tp, system, param) - if (any(tp%ldiscard)) then + if (any(tp%ldiscard(1:ntp))) then allocate(ldiscard, source=tp%ldiscard) - call tp%spill(system%tp_discards, ldiscard, ldestructive=.true.) + call tp%spill(system%tp_discards, ldiscard(1:ntp), ldestructive=.true.) end if end associate @@ -112,8 +115,9 @@ subroutine discard_cb_tp(tp, system, param) ! Internals integer(I4B) :: i real(DP) :: energy, vb2, rb2, rh2, rmin2, rmax2, rmaxu2 + character(len=STRMAX) :: idstr, timestr - associate(ntp => tp%nbody, cb => system%cb, t => param%t, Gmtot => system%Gmtot) + associate(ntp => tp%nbody, cb => system%cb, Gmtot => system%Gmtot) rmin2 = max(param%rmin * param%rmin, cb%radius * cb%radius) rmax2 = param%rmax**2 rmaxu2 = param%rmaxu**2 @@ -122,23 +126,32 @@ subroutine discard_cb_tp(tp, system, param) rh2 = dot_product(tp%xh(:, i), tp%xh(:, i)) if ((param%rmax >= 0.0_DP) .and. (rh2 > rmax2)) then tp%status(i) = DISCARDED_RMAX - write(*, *) "Particle ", tp%id(i), " too far from sun at t = ", t + write(idstr, *) tp%id(i) + write(timestr, *) param%t + write(*, *) "Particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " too far from the central body at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. tp%lmask(i) = .false. + call tp%info(i)%set_value(status="DISCARDED_RMAX", discard_time=param%t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i)) else if ((param%rmin >= 0.0_DP) .and. (rh2 < rmin2)) then tp%status(i) = DISCARDED_RMIN - write(*, *) "Particle ", tp%id(i), " too close to sun at t = ", t + write(idstr, *) tp%id(i) + write(timestr, *) param%t + write(*, *) "Particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " too close to the central body at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. tp%lmask(i) = .false. + call tp%info(i)%set_value(status="DISCARDED_RMIN", discard_time=param%t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i), discard_body_id=cb%id) else if (param%rmaxu >= 0.0_DP) then rb2 = dot_product(tp%xb(:, i), tp%xb(:, i)) vb2 = dot_product(tp%vb(:, i), tp%vb(:, i)) energy = 0.5_DP * vb2 - Gmtot / sqrt(rb2) if ((energy > 0.0_DP) .and. (rb2 > rmaxu2)) then tp%status(i) = DISCARDED_RMAXU - write(*, *) "Particle ", tp%id(i), " is unbound and too far from barycenter at t = ", t + write(idstr, *) tp%id(i) + write(timestr, *) param%t + write(*, *) "Particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " is unbound and too far from barycenter at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. tp%lmask(i) = .false. + call tp%info(i)%set_value(status="DISCARDED_RMAXU", discard_time=param%t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i)) end if end if end if @@ -166,6 +179,7 @@ subroutine discard_peri_tp(tp, system, param) integer(I4B) :: i, j, ih real(DP) :: r2 real(DP), dimension(NDIM) :: dx + character(len=STRMAX) :: idstr, timestr associate(cb => system%cb, ntp => tp%nbody, pl => system%pl, npl => system%pl%nbody, t => param%t) call tp%get_peri(system, param) @@ -183,8 +197,11 @@ subroutine discard_peri_tp(tp, system, param) (tp%atp(i) <= param%qmin_ahi) .and. & (tp%peri(i) <= param%qmin)) then tp%status(i) = DISCARDED_PERI - write(*, *) "Particle ", tp%id(i), " perihelion distance too small at t = ", t + write(idstr, *) tp%id(i) + write(timestr, *) param%t + write(*, *) "Particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " perihelion distance too small at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. + call tp%info(i)%set_value(status="DISCARDED_PERI", discard_time=param%t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i), discard_body_id=pl%id(j)) end if end if end if @@ -212,6 +229,7 @@ subroutine discard_pl_tp(tp, system, param) integer(I4B) :: i, j, isp real(DP) :: r2min, radius real(DP), dimension(NDIM) :: dx, dv + character(len=STRMAX) :: idstri, idstrj, timestr associate(ntp => tp%nbody, pl => system%pl, npl => system%pl%nbody, t => param%t, dt => param%dt) do i = 1, ntp @@ -225,8 +243,14 @@ subroutine discard_pl_tp(tp, system, param) tp%status(i) = DISCARDED_PLR tp%lmask(i) = .false. pl%ldiscard(j) = .true. - write(*, *) "Particle ", tp%id(i), " too close to massive body ", pl%id(j), " at t = ", t + write(idstri, *) tp%id(i) + write(idstrj, *) pl%id(j) + write(timestr, *) param%t + write(*, *) "Test particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstri)) // ")" & + // " too close to massive body " // trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstrj)) & + // " at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. + call tp%info(i)%set_value(status="DISCARDED_PLR", discard_time=param%t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i), discard_body_id=pl%id(j)) exit end if end do diff --git a/src/eucl/eucl.f90 b/src/eucl/eucl.f90 deleted file mode 100644 index af1646e4c..000000000 --- a/src/eucl/eucl.f90 +++ /dev/null @@ -1,38 +0,0 @@ -submodule (swiftest_classes) s_eucl - use swiftest -contains - - module subroutine eucl_dist_index_plpl(self) - !! author: Jacob R. Elliott and David A. Minton - !! - !! Turns i,j indices into k index for use in the Euclidean distance matrix - !! - !! Reference: - !! - !! Mélodie Angeletti, Jean-Marie Bonny, Jonas Koko. Parallel Euclidean distance matrix computation on big datasets *. - !! 2019. hal-0204751 - implicit none - ! Arguments - class(swiftest_pl), intent(inout) :: self !! Swiftest massive body objec - ! Internals - integer(I8B) :: i, j, counter, npl - - npl = int(self%nbody, kind=I8B) - associate(nplpl => self%nplpl) - nplpl = (npl * (npl - 1) / 2) ! number of entries in a strict lower triangle, nplm x npl, minus first column - if (allocated(self%k_plpl)) deallocate(self%k_plpl) ! Reset the index array if it's been set previously - allocate(self%k_plpl(2, nplpl)) - do i = 1, npl - counter = (i - 1_I8B) * npl - i * (i - 1_I8B) / 2_I8B + 1_I8B - do j = i + 1_I8B, npl - self%k_plpl(1, counter) = i - self%k_plpl(2, counter) = j - counter = counter + 1_I8B - end do - end do - end associate - - return - end subroutine eucl_dist_index_plpl - - end submodule s_eucl diff --git a/src/fraggle/fraggle_generate.f90 b/src/fraggle/fraggle_generate.f90 new file mode 100644 index 000000000..6f7ccb7a3 --- /dev/null +++ b/src/fraggle/fraggle_generate.f90 @@ -0,0 +1,567 @@ +submodule(fraggle_classes) s_fraggle_generate + use swiftest + + integer(I4B), parameter :: NFRAG_MIN = 7 !! The minimum allowable number of fragments (set to 6 because that's how many unknowns are needed in the tangential velocity calculation) + real(DP), parameter :: F_SPIN_FIRST = 0.05_DP !! The initial try value of the fraction of energy or momenum in spin (whichever has the lowest kinetic energy) + real(DP), parameter :: FRAGGLE_LTOL = 10 * epsilon(1.0_DP) + real(DP), parameter :: FRAGGLE_ETOL = 1e-8_DP + +contains + + module subroutine fraggle_generate_fragments(self, colliders, system, param, lfailure) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Generates a system of fragments in barycentric coordinates that conserves energy and momentum. + use, intrinsic :: ieee_exceptions + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle system object the outputs will be the fragmentation + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object containing the two-body equivalent values of the colliding bodies + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + logical, intent(out) :: lfailure !! Answers the question: Should this have been a merger instead? + ! Internals + integer(I4B) :: i + integer(I4B) :: try + real(DP) :: r_max_start, f_spin, dEtot, dLmag + integer(I4B), parameter :: MAXTRY = 100 + logical :: lk_plpl + logical, dimension(size(IEEE_ALL)) :: fpe_halting_modes, fpe_quiet_modes + logical, dimension(size(IEEE_USUAL)) :: fpe_flag + character(len=STRMAX) :: message + + ! The minimization and linear solvers can sometimes lead to floating point exceptions. Rather than halting the code entirely if this occurs, we + ! can simply fail the attempt and try again. So we need to turn off any floating point exception halting modes temporarily + call ieee_get_halting_mode(IEEE_ALL,fpe_halting_modes) ! Save the current halting modes so we can turn them off temporarily + fpe_quiet_modes(:) = .false. + call ieee_set_halting_mode(IEEE_ALL,fpe_quiet_modes) + + associate(frag => self, nfrag => self%nbody, pl => system%pl) + + write(message,*) nfrag + call fraggle_io_log_one_message("Fraggle generating " // trim(adjustl(message)) // " fragments.") + if (nfrag < NFRAG_MIN) then + write(message,*) "Fraggle needs at least ",NFRAG_MIN," fragments, but only ",nfrag," were given." + call fraggle_io_log_one_message(message) + lfailure = .true. + return + end if + f_spin = F_SPIN_FIRST + + lk_plpl = allocated(pl%k_plpl) + if (lk_plpl) deallocate(pl%k_plpl) + + call frag%set_natural_scale(colliders) + + call frag%reset() + + ! Calculate the initial energy of the system without the collisional family + call frag%get_energy_and_momentum(colliders, system, param, lbefore=.true.) + + ! Start out the fragments close to the initial separation distance. This will be increased if there is any overlap or we fail to find a solution + r_max_start = 1 * norm2(colliders%xb(:,2) - colliders%xb(:,1)) + lfailure = .false. + try = 1 + do while (try < MAXTRY) + write(message,*) try + call fraggle_io_log_one_message("Fraggle try " // trim(adjustl(message))) + if (lfailure) then + call frag%restructure(colliders, try, f_spin, r_max_start) + call frag%reset() + try = try + 1 + end if + + lfailure = .false. + call ieee_set_flag(ieee_all, .false.) ! Set all fpe flags to quiet + + call fraggle_generate_pos_vec(frag, colliders, r_max_start) + call frag%set_coordinate_system(colliders) + + ! Initial velocity guess will be the barycentric velocity of the colliding system so that the budgets are based on the much smaller collisional-frame velocities + do concurrent (i = 1:nfrag) + frag%vb(:, i) = frag%vbcom(:) + end do + + call frag%get_energy_and_momentum(colliders, system, param, lbefore=.false.) + call frag%set_budgets(colliders) + + call fraggle_generate_spins(frag, colliders, f_spin, lfailure) + if (lfailure) then + call fraggle_io_log_one_message("Fraggle failed to find spins") + cycle + end if + + call fraggle_generate_tan_vel(frag, colliders, lfailure) + if (lfailure) then + call fraggle_io_log_one_message("Fraggle failed to find tangential velocities") + cycle + end if + + call fraggle_generate_rad_vel(frag, colliders, lfailure) + if (lfailure) then + call fraggle_io_log_one_message("Fraggle failed to find radial velocities") + cycle + end if + + call frag%get_energy_and_momentum(colliders, system, param, lbefore=.false.) + dEtot = frag%Etot_after - frag%Etot_before + dLmag = .mag. (frag%Ltot_after(:) - frag%Ltot_before(:)) + + lfailure = ((abs(dEtot + frag%Qloss) > FRAGGLE_ETOL) .or. (dEtot > 0.0_DP)) + if (lfailure) then + write(message, *) dEtot, abs(dEtot + frag%Qloss) / FRAGGLE_ETOL + call fraggle_io_log_one_message("Fraggle failed due to high energy error: " // trim(adjustl(message))) + cycle + end if + + lfailure = ((abs(dLmag) / (.mag.frag%Ltot_before)) > FRAGGLE_LTOL) + if (lfailure) then + write(message,*) dLmag / (.mag.frag%Ltot_before(:)) + call fraggle_io_log_one_message("Fraggle failed due to high angular momentum error: " // trim(adjustl(message))) + cycle + end if + + ! Check if any of the usual floating point exceptions happened, and fail the try if so + call ieee_get_flag(ieee_usual, fpe_flag) + lfailure = any(fpe_flag) + if (.not.lfailure) exit + write(message,*) "Fraggle failed due to a floating point exception: ", fpe_flag + call fraggle_io_log_one_message(message) + end do + + write(message,*) try + if (lfailure) then + call fraggle_io_log_one_message("Fraggle fragment generation failed after " // trim(adjustl(message)) // " tries") + else + call fraggle_io_log_one_message("Fraggle fragment generation succeeded after " // trim(adjustl(message)) // " tries") + call fraggle_io_log_generate(frag) + end if + + call frag%set_original_scale(colliders) + + ! Restore the big array + if (lk_plpl) call pl%index(param) + end associate + call ieee_set_halting_mode(IEEE_ALL,fpe_halting_modes) ! Save the current halting modes so we can turn them off temporarily + + return + end subroutine fraggle_generate_fragments + + + subroutine fraggle_generate_pos_vec(frag, colliders, r_max_start) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Initializes the orbits of the fragments around the center of mass. The fragments are initially placed on a plane defined by the + !! pre-impact angular momentum. They are distributed on an ellipse surrounding the center of mass. + !! The initial positions do not conserve energy or momentum, so these need to be adjusted later. + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + real(DP), intent(in) :: r_max_start !! Initial guess for the starting maximum radial distance of fragments + ! Internals + real(DP) :: dis, rad, r_max + logical, dimension(:), allocatable :: loverlap + integer(I4B) :: i, j + + associate(nfrag => frag%nbody) + allocate(loverlap(nfrag)) + + ! Place the fragments into a region that is big enough that we should usually not have overlapping bodies + ! An overlapping bodies will collide in the next time step, so it's not a major problem if they do (it just slows the run down) + r_max = r_max_start + rad = sum(colliders%radius(:)) + + ! We will treat the first two fragments of the list as special cases. They get initialized the maximum distances apart along the original impactor distance vector. + ! This is done because in a regular disruption, the first body is the largest, the second the second largest, and the rest are smaller equal-mass fragments. + + call random_number(frag%x_coll(:,3:nfrag)) + loverlap(:) = .true. + do while (any(loverlap(3:nfrag))) + frag%x_coll(:, 1) = colliders%xb(:, 1) - frag%xbcom(:) + frag%x_coll(:, 2) = colliders%xb(:, 2) - frag%xbcom(:) + r_max = r_max + 0.1_DP * rad + do i = 3, nfrag + if (loverlap(i)) then + call random_number(frag%x_coll(:,i)) + frag%x_coll(:, i) = 2 * (frag%x_coll(:, i) - 0.5_DP) * r_max + end if + end do + loverlap(:) = .false. + do j = 1, nfrag + do i = j + 1, nfrag + dis = norm2(frag%x_coll(:,j) - frag%x_coll(:,i)) + loverlap(i) = loverlap(i) .or. (dis <= (frag%radius(i) + frag%radius(j))) + end do + end do + end do + call fraggle_util_shift_vector_to_origin(frag%mass, frag%x_coll) + call frag%set_coordinate_system(colliders) + + do i = 1, nfrag + frag%xb(:,i) = frag%x_coll(:,i) + frag%xbcom(:) + end do + + frag%xbcom(:) = 0.0_DP + do i = 1, nfrag + frag%xbcom(:) = frag%xbcom(:) + frag%mass(i) * frag%xb(:,i) + end do + frag%xbcom(:) = frag%xbcom(:) / frag%mtot + end associate + + return + end subroutine fraggle_generate_pos_vec + + + subroutine fraggle_generate_spins(frag, colliders, f_spin, lfailure) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Calculates the spins of a collection of fragments such that they conserve angular momentum without blowing the fragment kinetic energy budget. + !! + !! A failure will trigger a restructuring of the fragments so we will try new values of the radial position distribution. + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + real(DP), intent(in) :: f_spin !! Fraction of energy or momentum that goes into spin (whichever gives the lowest kinetic energy) + logical, intent(out) :: lfailure !! Logical flag indicating whether this step fails or succeeds! + ! Internals + real(DP), dimension(NDIM) :: L_remainder, rot_L, rot_ke + integer(I4B) :: i + character(len=STRMAX) :: message + + associate(nfrag => frag%nbody) + lfailure = .false. + + ! Start the first two bodies with the same rotation as the original two impactors, then distribute the remaining angular momentum among the rest + L_remainder(:) = frag%L_budget(:) + frag%rot(:,:) = 0.0_DP + + frag%ke_spin = 0.0_DP + do i = 1, nfrag + ! Convert a fraction (f_spin) of either the remaining angular momentum or kinetic energy budget into spin, whichever gives the smaller rotation so as not to blow any budgets + rot_ke(:) = sqrt(2 * f_spin * frag%ke_budget / (nfrag * frag%mass(i) * frag%radius(i)**2 * frag%Ip(3, i))) * L_remainder(:) / norm2(L_remainder(:)) + rot_L(:) = f_spin * L_remainder(:) / (nfrag * frag%mass(i) * frag%radius(i)**2 * frag%Ip(3, i)) + if (norm2(rot_ke) < norm2(rot_L)) then + frag%rot(:,i) = rot_ke(:) + else + frag%rot(:, i) = rot_L(:) + end if + frag%ke_spin = frag%ke_spin + frag%mass(i) * frag%Ip(3, i) * frag%radius(i)**2 * dot_product(frag%rot(:, i), frag%rot(:, i)) + end do + frag%ke_spin = 0.5_DP * frag%ke_spin + + lfailure = ((frag%ke_budget - frag%ke_spin - frag%ke_orbit) < 0.0_DP) + + if (lfailure) then + call fraggle_io_log_one_message(" ") + call fraggle_io_log_one_message("Spin failure diagnostics") + write(message, *) frag%ke_budget + call fraggle_io_log_one_message("ke_budget : " // trim(adjustl(message))) + write(message, *) frag%ke_spin + call fraggle_io_log_one_message("ke_spin : " // trim(adjustl(message))) + write(message, *) frag%ke_orbit + call fraggle_io_log_one_message("ke_orbit : " // trim(adjustl(message))) + write(message, *) frag%ke_budget - frag%ke_spin - frag%ke_orbit + call fraggle_io_log_one_message("ke_remainder : " // trim(adjustl(message))) + end if + + end associate + + return + end subroutine fraggle_generate_spins + + + subroutine fraggle_generate_tan_vel(frag, colliders, lfailure) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Adjusts the tangential velocities and spins of a collection of fragments such that they conserve angular momentum without blowing the fragment kinetic energy budget. + !! This procedure works in several stages, with a goal to solve the angular and linear momentum constraints on the fragments, while still leaving a positive balance of + !! our fragment kinetic energy (frag%ke_budget) that we can put into the radial velocity distribution. + !! + !! The first thing we'll try to do is solve for the tangential velocities of the first 6 fragments, using angular and linear momentum as constraints and an initial + !! tangential velocity distribution for the remaining bodies (if there are any) that distributes their angular momentum equally between them. + !! If that doesn't work and we blow our kinetic energy budget, we will attempt to find a tangential velocity distribution that minimizes the kinetic energy while + !! conserving momentum. + !! + !! A failure will trigger a restructuring of the fragments so we will try new values of the radial position distribution. + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + logical, intent(out) :: lfailure !! Logical flag indicating whether this step fails or succeeds + ! Internals + integer(I4B) :: i + real(DP), parameter :: TOL_MIN = 1e-1_DP ! This doesn't have to be very accurate, as we really just want a tangential velocity distribution with less kinetic energy than our initial guess. + real(DP), parameter :: TOL_INIT = 1e-14_DP + real(DP), parameter :: VNOISE_MAG = 1e-3_DP !! Magnitude of the noise to apply to initial conditions to help minimizer find a solution in case of failure + integer(I4B), parameter :: MAXLOOP = 10 + real(DP) :: tol, ke_remainder + real(DP), dimension(:), allocatable :: v_t_initial + real(DP), dimension(frag%nbody) :: kefrag, vnoise + type(lambda_obj) :: spinfunc + type(lambda_obj_err) :: objective_function + real(DP), dimension(NDIM) :: Li, L_remainder, L_frag_tot + character(len=STRMAX) :: message + + associate(nfrag => frag%nbody) + lfailure = .false. + + allocate(v_t_initial, mold=frag%v_t_mag) + v_t_initial(:) = 0.0_DP + frag%v_coll(:,:) = 0.0_DP + + ! Next we will solve for the tangential component of the velocities that both conserves linear momentum and uses the remaining angular momentum not used in spin. + ! This will be done using a linear solver that solves for the tangential velocities of the first 6 fragments, constrained by the linear and angular momentum vectors, + ! which is embedded in a non-linear minimizer that will adjust the tangential velocities of the remaining i>6 fragments to minimize kinetic energy for a given momentum solution + ! The initial conditions fed to the minimizer for the fragments will be the remaining angular momentum distributed between the fragments. + call frag%get_ang_mtm() + L_remainder(:) = frag%L_budget(:) - frag%L_spin(:) + do i = 1, nfrag + v_t_initial(i) = norm2(L_remainder(:)) / ((nfrag - i + 1) * frag%mass(i) * norm2(frag%x_coll(:,i))) + Li(:) = frag%mass(i) * (frag%x_coll(:,i) .cross. (v_t_initial(i) * frag%v_t_unit(:, i))) + L_remainder(:) = L_remainder(:) - Li(:) + end do + + ! Find the local kinetic energy minimum for the system that conserves linear and angular momentum + objective_function = lambda_obj(tangential_objective_function, lfailure) + + tol = TOL_INIT + do while(tol < TOL_MIN) + frag%v_t_mag(7:nfrag) = util_minimize_bfgs(objective_function, nfrag-6, v_t_initial(7:nfrag), tol, MAXLOOP, lfailure) + ! Now that the KE-minimized values of the i>6 fragments are found, calculate the momentum-conserving solution for tangential velociteis + v_t_initial(7:nfrag) = frag%v_t_mag(7:nfrag) + if (.not.lfailure) exit + tol = tol * 2_DP ! Keep increasing the tolerance until we converge on a solution + call random_number(vnoise(1:nfrag)) ! Adding a bit of noise to the initial conditions helps it find a solution more often + vnoise(:) = 1.0_DP + VNOISE_MAG * (2 * vnoise(:) - 1._DP) + v_t_initial(:) = v_t_initial(:) * vnoise(:) + end do + frag%v_t_mag(1:nfrag) = solve_fragment_tan_vel(v_t_mag_input=v_t_initial(7:nfrag), lfailure=lfailure) + + ! Perform one final shift of the radial velocity vectors to align with the center of mass of the collisional system (the origin) + frag%vb(:,1:nfrag) = fraggle_util_vmag_to_vb(frag%v_r_mag(1:nfrag), frag%v_r_unit(:,1:nfrag), frag%v_t_mag(1:nfrag), frag%v_t_unit(:,1:nfrag), frag%mass(1:nfrag), frag%vbcom(:)) + do concurrent (i = 1:nfrag) + frag%v_coll(:,i) = frag%vb(:,i) - frag%vbcom(:) + end do + + ! Now do a kinetic energy budget check to make sure we are still within the budget. + kefrag = 0.0_DP + do concurrent(i = 1:nfrag) + kefrag(i) = frag%mass(i) * dot_product(frag%vb(:, i), frag%vb(:, i)) + end do + frag%ke_orbit = 0.5_DP * sum(kefrag(:)) + + ! If we are over the energy budget, flag this as a failure so we can try again + lfailure = ((frag%ke_budget - frag%ke_spin - frag%ke_orbit) < 0.0_DP) + if (lfailure) then + call fraggle_io_log_one_message(" ") + call fraggle_io_log_one_message("Tangential velocity failure diagnostics") + call frag%get_ang_mtm() + L_frag_tot = frag%L_spin(:) + frag%L_orbit(:) + write(message, *) .mag.(frag%L_budget(:) - L_frag_tot(:)) / (.mag.frag%Ltot_before(:)) + call fraggle_io_log_one_message("|L_remainder| : " // trim(adjustl(message))) + write(message, *) frag%ke_budget + call fraggle_io_log_one_message("ke_budget : " // trim(adjustl(message))) + write(message, *) frag%ke_spin + call fraggle_io_log_one_message("ke_spin : " // trim(adjustl(message))) + write(message, *) frag%ke_orbit + call fraggle_io_log_one_message("ke_tangential : " // trim(adjustl(message))) + write(message, *) frag%ke_budget - frag%ke_spin - frag%ke_orbit + call fraggle_io_log_one_message("ke_radial : " // trim(adjustl(message))) + end if + end associate + + return + + contains + function solve_fragment_tan_vel(lfailure, v_t_mag_input) result(v_t_mag_output) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Adjusts the positions, velocities, and spins of a collection of fragments such that they conserve angular momentum + implicit none + ! Arguments + logical, intent(out) :: lfailure !! Error flag + real(DP), dimension(:), optional, intent(in) :: v_t_mag_input !! Unknown tangential velocities for fragments 7:nfrag + ! Internals + integer(I4B) :: i + ! Result + real(DP), dimension(:), allocatable :: v_t_mag_output + + real(DP), dimension(2 * NDIM, 2 * NDIM) :: A ! LHS of linear equation used to solve for momentum constraint in Gauss elimination code + real(DP), dimension(2 * NDIM) :: b ! RHS of linear equation used to solve for momentum constraint in Gauss elimination code + real(DP), dimension(NDIM) :: L_lin_others, L_orb_others, L, vtmp + + associate(nfrag => frag%nbody) + lfailure = .false. + ! We have 6 constraint equations (2 vector constraints in 3 dimensions each) + ! The first 3 are that the linear momentum of the fragments is zero with respect to the collisional barycenter + ! The second 3 are that the sum of the angular momentum of the fragments is conserved from the pre-impact state + L_lin_others(:) = 0.0_DP + L_orb_others(:) = 0.0_DP + do i = 1, nfrag + if (i <= 2 * NDIM) then ! The tangential velocities of the first set of bodies will be the unknowns we will solve for to satisfy the constraints + A(1:3, i) = frag%mass(i) * frag%v_t_unit(:, i) + A(4:6, i) = frag%mass(i) * frag%rmag(i) * (frag%v_r_unit(:, i) .cross. frag%v_t_unit(:, i)) + else if (present(v_t_mag_input)) then + vtmp(:) = v_t_mag_input(i - 6) * frag%v_t_unit(:, i) + L_lin_others(:) = L_lin_others(:) + frag%mass(i) * vtmp(:) + L(:) = frag%mass(i) * (frag%x_coll(:, i) .cross. vtmp(:)) + L_orb_others(:) = L_orb_others(:) + L(:) + end if + end do + b(1:3) = -L_lin_others(:) + b(4:6) = frag%L_budget(:) - frag%L_spin(:) - L_orb_others(:) + allocate(v_t_mag_output(nfrag)) + v_t_mag_output(1:6) = util_solve_linear_system(A, b, 6, lfailure) + if (present(v_t_mag_input)) v_t_mag_output(7:nfrag) = v_t_mag_input(:) + end associate + return + end function solve_fragment_tan_vel + + + function tangential_objective_function(v_t_mag_input, lfailure) result(fval) + !! Author: David A. Minton + !! + !! Objective function for evaluating how close our fragment velocities get to minimizing KE error from our required value + implicit none + ! Arguments + real(DP), dimension(:), intent(in) :: v_t_mag_input !! Unknown tangential component of velocity vector set previously by angular momentum constraint + logical, intent(out) :: lfailure !! Error flag + ! Result + real(DP) :: fval + ! Internals + integer(I4B) :: i + real(DP), dimension(NDIM,frag%nbody) :: v_shift + real(DP), dimension(frag%nbody) :: v_t_new, kearr + real(DP) :: keo + + associate(nfrag => frag%nbody) + lfailure = .false. + + v_t_new(:) = solve_fragment_tan_vel(v_t_mag_input=v_t_mag_input(:), lfailure=lfailure) + v_shift(:,:) = fraggle_util_vmag_to_vb(frag%v_r_mag, frag%v_r_unit, v_t_new, frag%v_t_unit, frag%mass, frag%vbcom) + + kearr = 0.0_DP + do concurrent(i = 1:nfrag) + kearr(i) = frag%mass(i) * dot_product(v_shift(:, i), v_shift(:, i)) + end do + keo = 0.5_DP * sum(kearr(:)) + fval = keo + lfailure = .false. + end associate + + return + end function tangential_objective_function + + end subroutine fraggle_generate_tan_vel + + + subroutine fraggle_generate_rad_vel(frag, colliders, lfailure) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! + !! Adjust the fragment velocities to set the fragment orbital kinetic energy. This will minimize the difference between the fragment kinetic energy and the energy budget + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + logical, intent(out) :: lfailure !! Logical flag indicating whether this step fails or succeeds! + ! Internals + real(DP), parameter :: TOL_MIN = FRAGGLE_ETOL ! This needs to be more accurate than the tangential step, as we are trying to minimize the total residual energy + real(DP), parameter :: TOL_INIT = 1e-14_DP + real(DP), parameter :: VNOISE_MAG = 1e-10_DP !! Magnitude of the noise to apply to initial conditions to help minimizer find a solution in case of failure + integer(I4B), parameter :: MAXLOOP = 100 + real(DP) :: ke_radial, tol + integer(I4B) :: i, j + real(DP), dimension(:), allocatable :: v_r_initial + real(DP), dimension(:,:), allocatable :: v_r + real(DP), dimension(frag%nbody) :: vnoise + type(lambda_obj) :: objective_function + character(len=STRMAX) :: message + + associate(nfrag => frag%nbody) + ! Set the "target" ke for the radial component + ke_radial = frag%ke_budget - frag%ke_spin - frag%ke_orbit + + allocate(v_r_initial, source=frag%v_r_mag) + ! Initialize radial velocity magnitudes with a random value that related to equipartition of kinetic energy with some noise + call random_number(vnoise(1:nfrag)) + vnoise(:) = 1.0_DP + VNOISE_MAG * (2 * vnoise(:) - 1.0_DP) + v_r_initial(1:nfrag) = sqrt(abs(2 * ke_radial) / (frag%mass(1:nfrag) * nfrag)) * vnoise(1:nfrag) + + ! Initialize the lambda function using a structure constructor that calls the init method + ! Minimize the ke objective function using the BFGS optimizer + objective_function = lambda_obj(radial_objective_function) + tol = TOL_INIT + do while(tol < TOL_MIN) + frag%v_r_mag = util_minimize_bfgs(objective_function, nfrag, v_r_initial, tol, MAXLOOP, lfailure) + if (.not.lfailure) exit + tol = tol * 2 ! Keep increasing the tolerance until we converge on a solution + v_r_initial(:) = frag%v_r_mag(:) + call random_number(vnoise(1:nfrag)) ! Adding a bit of noise to the initial conditions helps it find a solution more often + vnoise(:) = 1.0_DP + VNOISE_MAG * (2 * vnoise(:) - 1._DP) + v_r_initial(:) = v_r_initial(:) * vnoise(:) + end do + + ! Shift the radial velocity vectors to align with the center of mass of the collisional system (the origin) + frag%ke_orbit = 0.0_DP + frag%vb(:,1:nfrag) = fraggle_util_vmag_to_vb(frag%v_r_mag(1:nfrag), frag%v_r_unit(:,1:nfrag), frag%v_t_mag(1:nfrag), frag%v_t_unit(:,1:nfrag), frag%mass(1:nfrag), frag%vbcom(:)) + do i = 1, nfrag + frag%v_coll(:, i) = frag%vb(:, i) - frag%vbcom(:) + frag%ke_orbit = frag%ke_orbit + frag%mass(i) * dot_product(frag%vb(:, i), frag%vb(:, i)) + end do + frag%ke_orbit = 0.5_DP * frag%ke_orbit + + lfailure = abs((frag%ke_budget - (frag%ke_orbit + frag%ke_spin)) / frag%ke_budget) > FRAGGLE_ETOL + if (lfailure) then + call fraggle_io_log_one_message(" ") + call fraggle_io_log_one_message("Radial velocity failure diagnostics") + write(message, *) frag%ke_budget + call fraggle_io_log_one_message("ke_budget : " // trim(adjustl(message))) + write(message, *) frag%ke_spin + call fraggle_io_log_one_message("ke_spin : " // trim(adjustl(message))) + write(message, *) frag%ke_orbit + call fraggle_io_log_one_message("ke_orbit : " // trim(adjustl(message))) + write(message, *) frag%ke_budget - (frag%ke_orbit + frag%ke_spin) + call fraggle_io_log_one_message("ke_remainder : " // trim(adjustl(message))) + end if + + end associate + return + + contains + function radial_objective_function(v_r_mag_input) result(fval) + !! Author: David A. Minton + !! + !! Objective function for evaluating how close our fragment velocities get to minimizing KE error from our required value + implicit none + ! Arguments + real(DP), dimension(:), intent(in) :: v_r_mag_input !! Unknown radial component of fragment velocity vector + ! Result + real(DP) :: fval !! The objective function result, which is the square of the difference between the calculated fragment kinetic energy and our target + !! Minimizing this brings us closer to our objective + ! Internals + integer(I4B) :: i + real(DP), dimension(:,:), allocatable :: v_shift + real(DP), dimension(frag%nbody) :: kearr + real(DP) :: keo, ke_radial + + associate(nfrag => frag%nbody) + allocate(v_shift, mold=frag%vb) + v_shift(:,:) = fraggle_util_vmag_to_vb(v_r_mag_input, frag%v_r_unit, frag%v_t_mag, frag%v_t_unit, frag%mass, frag%vbcom) + do concurrent(i = 1:nfrag) + kearr(i) = frag%mass(i) * (frag%Ip(3, i) * frag%radius(i)**2 * dot_product(frag%rot(:, i), frag%rot(:, i)) + dot_product(v_shift(:, i), v_shift(:, i))) + end do + keo = 2 * frag%ke_budget - sum(kearr(:)) + ke_radial = frag%ke_budget - frag%ke_orbit - frag%ke_spin + ! The following ensures that fval = 0 is a local minimum, which is what the BFGS method is searching for + fval = (keo / (2 * ke_radial))**2 + end associate + + return + end function radial_objective_function + + end subroutine fraggle_generate_rad_vel + +end submodule s_fraggle_generate diff --git a/src/fraggle/fraggle_io.f90 b/src/fraggle/fraggle_io.f90 new file mode 100644 index 000000000..dbd721216 --- /dev/null +++ b/src/fraggle/fraggle_io.f90 @@ -0,0 +1,255 @@ +submodule(fraggle_classes) s_fraggle_io + use swiftest + +contains + + module subroutine fraggle_io_log_generate(frag) + !! author: David A. Minton + !! + !! Writes a log of the results of the fragment generation + implicit none + ! Arguments + class(fraggle_fragments), intent(in) :: frag + ! Internals + integer(I4B) :: i + character(STRMAX) :: errmsg + character(len=*), parameter :: fmtlabel = "(A14,10(ES11.4,1X,:))" + + open(unit=FRAGGLE_LOG_UNIT, file=FRAGGLE_LOG_OUT, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *, err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, *) " Fraggle fragment generation results" + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, "(' dL_tot should be very small' )") + write(FRAGGLE_LOG_UNIT,fmtlabel) ' dL_tot |', (.mag.(frag%Ltot_after(:) - frag%Ltot_before(:))) / (.mag.frag%Ltot_before(:)) + write(FRAGGLE_LOG_UNIT, "(' dE_tot should be negative and equal to Qloss' )") + write(FRAGGLE_LOG_UNIT,fmtlabel) ' dE_tot |', (frag%Etot_after - frag%Etot_before) / abs(frag%Etot_before) + write(FRAGGLE_LOG_UNIT,fmtlabel) ' Qloss |', -frag%Qloss / abs(frag%Etot_before) + write(FRAGGLE_LOG_UNIT,fmtlabel) ' dE - Qloss |', (frag%Etot_after - frag%Etot_before + frag%Qloss) / abs(frag%Etot_before) + write(FRAGGLE_LOG_UNIT, "(' -------------------------------------------------------------------------------------')") + write(FRAGGLE_LOG_UNIT, *) "Individual fragment values (collisional system natural units)" + write(FRAGGLE_LOG_UNIT, *) "mass" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%mass(i) + end do + write(FRAGGLE_LOG_UNIT, *) "x_coll" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%x_coll(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "v_coll" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%v_coll(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "xb" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%xb(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "vb" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%vb(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "rot" + do i = 1, frag%nbody + write(FRAGGLE_LOG_UNIT, *) i, frag%rot(:,i) + end do + + close(FRAGGLE_LOG_UNIT) + + return + 667 continue + write(*,*) "Error writing Fraggle message to log file: " // trim(adjustl(errmsg)) + end subroutine fraggle_io_log_generate + + + module subroutine fraggle_io_log_one_message(message) + !! author: David A. Minton + !! + !! Writes a single message to the fraggle log file + implicit none + ! Arguments + character(len=*), intent(in) :: message + ! Internals + character(STRMAX) :: errmsg + + open(unit=FRAGGLE_LOG_UNIT, file=FRAGGLE_LOG_OUT, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *) trim(adjustl(message)) + close(FRAGGLE_LOG_UNIT) + + return + 667 continue + write(*,*) "Error writing Fraggle message to log file: " // trim(adjustl(errmsg)) + end subroutine fraggle_io_log_one_message + + + module subroutine fraggle_io_log_pl(pl, param) + !! author: David A. Minton + !! + !! Writes a single message to the fraggle log file + implicit none + ! Arguments + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object (only the new bodies generated in a collision) + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + ! Internals + integer(I4B) :: i + character(STRMAX) :: errmsg + + open(unit=FRAGGLE_LOG_UNIT, file=FRAGGLE_LOG_OUT, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *, err = 667, iomsg = errmsg) + + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, *) " Fraggle fragment final body properties" + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, *) "id, name" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%id(i), pl%info(i)%name + end do + write(FRAGGLE_LOG_UNIT, *) "mass, Gmass" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%mass(i), pl%Gmass(i) + end do + write(FRAGGLE_LOG_UNIT, *) "radius" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%radius(i) + end do + write(FRAGGLE_LOG_UNIT, *) "xb" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%xb(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "vb" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%vb(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "xh" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%xh(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "vh" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%vh(:,i) + end do + + if (param%lrotation) then + write(FRAGGLE_LOG_UNIT, *) "rot" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%rot(:,i) + end do + write(FRAGGLE_LOG_UNIT, *) "Ip" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%Ip(:,i) + end do + end if + + if (param%ltides) then + write(FRAGGLE_LOG_UNIT, *) "Q" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%Q(i) + end do + write(FRAGGLE_LOG_UNIT, *) "k2" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%k2(i) + end do + write(FRAGGLE_LOG_UNIT, *) "tlag" + do i = 1, pl%nbody + write(FRAGGLE_LOG_UNIT, *) i, pl%tlag(i) + end do + end if + + close(FRAGGLE_LOG_UNIT) + + return + 667 continue + write(*,*) "Error writing Fraggle message to log file: " // trim(adjustl(errmsg)) + end subroutine fraggle_io_log_pl + + + module subroutine fraggle_io_log_regime(colliders, frag) + !! author: David A. Minton + !! + !! Writes a log of the results of the collisional regime determination + implicit none + ! Arguments + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + class(fraggle_fragments), intent(in) :: frag !! Fraggle fragment object + ! Internals + character(STRMAX) :: errmsg + + open(unit=FRAGGLE_LOG_UNIT, file=FRAGGLE_LOG_OUT, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *, err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, *) " Fraggle collisional regime determination results" + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + write(FRAGGLE_LOG_UNIT, *) "----------------------- Collider information -----------------------" + write(FRAGGLE_LOG_UNIT, *) "True number of colliders : ",colliders%ncoll + write(FRAGGLE_LOG_UNIT, *) "Index list of true colliders : ",colliders%idx(1:colliders%ncoll) + write(FRAGGLE_LOG_UNIT, *) "-------------------- Two-body equialent values ---------------------" + write(FRAGGLE_LOG_UNIT, *) "mass1 : ",colliders%mass(1) + write(FRAGGLE_LOG_UNIT, *) "radius1 : ",colliders%radius(1) + write(FRAGGLE_LOG_UNIT, *) "xb1 : ",colliders%xb(:,1) + write(FRAGGLE_LOG_UNIT, *) "vb1 : ",colliders%vb(:,1) + write(FRAGGLE_LOG_UNIT, *) "rot1 : ",colliders%rot(:,1) + write(FRAGGLE_LOG_UNIT, *) "Ip1 : ",colliders%Ip(:,1) + write(FRAGGLE_LOG_UNIT, *) "L_spin1 : ",colliders%L_spin(:,1) + write(FRAGGLE_LOG_UNIT, *) "L_orbit1 : ",colliders%L_orbit(:,1) + write(FRAGGLE_LOG_UNIT, *) "mass2 : ",colliders%mass(2) + write(FRAGGLE_LOG_UNIT, *) "radius2 : ",colliders%radius(2) + write(FRAGGLE_LOG_UNIT, *) "xb2 : ",colliders%xb(:,2) + write(FRAGGLE_LOG_UNIT, *) "vb2 : ",colliders%vb(:,2) + write(FRAGGLE_LOG_UNIT, *) "rot2 : ",colliders%rot(:,2) + write(FRAGGLE_LOG_UNIT, *) "Ip2 : ",colliders%Ip(:,2) + write(FRAGGLE_LOG_UNIT, *) "L_spin2 : ",colliders%L_spin(:,2) + write(FRAGGLE_LOG_UNIT, *) "L_orbit2 : ",colliders%L_orbit(:,2) + write(FRAGGLE_LOG_UNIT, *) "------------------------------ Regime -----------------------------" + select case(frag%regime) + case(COLLRESOLVE_REGIME_MERGE) + write(FRAGGLE_LOG_UNIT, *) "Merge" + case(COLLRESOLVE_REGIME_DISRUPTION) + write(FRAGGLE_LOG_UNIT, *) "Disruption" + case(COLLRESOLVE_REGIME_SUPERCATASTROPHIC) + write(FRAGGLE_LOG_UNIT, *) "Supercatastrophic disruption" + case(COLLRESOLVE_REGIME_GRAZE_AND_MERGE) + write(FRAGGLE_LOG_UNIT, *) "Graze and merge" + case(COLLRESOLVE_REGIME_HIT_AND_RUN) + write(FRAGGLE_LOG_UNIT, *) "Hit and run" + end select + write(FRAGGLE_LOG_UNIT, *) "----------------------- Fragment information ----------------------" + write(FRAGGLE_LOG_UNIT, *) "Total mass of fragments : ", frag%mtot + write(FRAGGLE_LOG_UNIT, *) "Largest fragment mass : ", frag%mass_dist(1) + write(FRAGGLE_LOG_UNIT, *) "Second-largest fragment mass : ", frag%mass_dist(2) + write(FRAGGLE_LOG_UNIT, *) "Remaining fragment mass : ", frag%mass_dist(3) + write(FRAGGLE_LOG_UNIT, *) "Center of mass position : ", frag%xbcom(:) + write(FRAGGLE_LOG_UNIT, *) "Center of mass velocity : ", frag%vbcom(:) + write(FRAGGLE_LOG_UNIT, *) "Energy loss : ", frag%Qloss + write(FRAGGLE_LOG_UNIT, *) "--------------------------------------------------------------------" + close(FRAGGLE_LOG_UNIT) + + return + 667 continue + write(*,*) "Error writing Fraggle regime information to log file: " // trim(adjustl(errmsg)) + end subroutine fraggle_io_log_regime + + + module subroutine fraggle_io_log_start(param) + !! author: David A. Minton + !! + !! Checks to see if the Fraggle log file needs to be replaced if this is a new run, or appended if this is a restarted run + implicit none + ! Arguments + class(swiftest_parameters), intent(in) :: param + ! Internals + character(STRMAX) :: errmsg + logical :: fileExists + + inquire(file=FRAGGLE_LOG_OUT, exist=fileExists) + if (.not.param%lrestart .or. .not.fileExists) then + open(unit=FRAGGLE_LOG_UNIT, file=FRAGGLE_LOG_OUT, status="REPLACE", err = 667, iomsg = errmsg) + write(FRAGGLE_LOG_UNIT, *, err = 667, iomsg = errmsg) "Fraggle logfile" + end if + close(FRAGGLE_LOG_UNIT) + + return + + 667 continue + write(*,*) "Error writing Fraggle log file: " // trim(adjustl(errmsg)) + end subroutine fraggle_io_log_start + +end submodule s_fraggle_io \ No newline at end of file diff --git a/src/fraggle/fraggle_placeholder.f90 b/src/fraggle/fraggle_placeholder.f90 new file mode 100644 index 000000000..bbf08bb04 --- /dev/null +++ b/src/fraggle/fraggle_placeholder.f90 @@ -0,0 +1,44 @@ +submodule(fraggle_classes) s_fraggle_placeholder + use swiftest + +contains + + !> The following interfaces are placeholders intended to satisfy the required abstract methods given by the parent class + module subroutine fraggle_placeholder_accel(self, system, param, t, lbeg) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Current simulation time + logical, intent(in) :: lbeg !! Optional argument that determines whether or not this is the beginning or end of the step + write(*,*) "The type-bound procedure 'accel' is not defined for type fraggle_fragments" + return + end subroutine fraggle_placeholder_accel + + module subroutine fraggle_placeholder_kick(self, system, param, t, dt, lbeg) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system objec + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Current time + real(DP), intent(in) :: dt !! Stepsize + logical, intent(in) :: lbeg !! Logical flag indicating whether this is the beginning of the half step or not. + + write(*,*) "The type-bound procedure 'kick' is not defined for type fraggle_fragments" + return + end subroutine fraggle_placeholder_kick + + module subroutine fraggle_placeholder_step(self, system, param, t, dt) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Swiftest body object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Simulation time + real(DP), intent(in) :: dt !! Current stepsize + + write(*,*) "The type-bound procedure 'step' is not defined for type fraggle_fragments" + return + end subroutine fraggle_placeholder_step + + +end submodule s_fraggle_placeholder \ No newline at end of file diff --git a/src/fraggle/fraggle_regime.f90 b/src/fraggle/fraggle_regime.f90 new file mode 100644 index 000000000..df9265ae7 --- /dev/null +++ b/src/fraggle/fraggle_regime.f90 @@ -0,0 +1,368 @@ +submodule(fraggle_classes) s_fraggle_regime + use swiftest + +contains + + module subroutine fraggle_regime_colliders(self, frag, system, param) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Determine which fragmentation regime the set of colliders will be. This subroutine is a wrapper for the non-polymorphic raggle_regime_collresolve subroutine. + !! It converts to SI units prior to calling + implicit none + ! Arguments + class(fraggle_colliders), intent(inout) :: self !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(swiftest_nbody_system), intent(in) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current Swiftest run configuration parameters + ! Internals + integer(I4B) :: jtarg, jproj, regime + real(DP), dimension(2) :: radius_si, mass_si, density_si + real(DP) :: min_mfrag_si, Mcb_si + real(DP), dimension(NDIM) :: x1_si, v1_si, x2_si, v2_si + real(DP) :: mlr, mslr, mtot, dentot, msys, msys_new, Qloss, impact_parameter + logical :: fileExists + + associate(colliders => self) + ! Convert all quantities to SI units and determine which of the pair is the projectile vs. target before sending them to the regime determination subroutine + if (colliders%mass(1) > colliders%mass(2)) then + jtarg = 1 + jproj = 2 + else + jtarg = 2 + jproj = 1 + end if + mass_si(:) = colliders%mass([jtarg, jproj]) * param%MU2KG !! The two-body equivalent masses of the collider system + radius_si(:) = colliders%radius([jtarg, jproj]) * param%DU2M !! The two-body equivalent radii of the collider system + density_si(:) = mass_si(:) / (4.0_DP / 3._DP * PI * radius_si(:)**3) !! The two-body equivalent density of the collider system + x1_si(:) = colliders%xb(:,jtarg) * param%DU2M !! The first body of the two-body equivalent position vector the collider system + v1_si(:) = colliders%vb(:,jtarg) * param%DU2M / param%TU2S !! The first body of the two-body equivalent velocity vector the collider system + x2_si(:) = colliders%xb(:,jproj) * param%DU2M !! The second body of the two-body equivalent position vector the collider system + v2_si(:) = colliders%vb(:,jproj) * param%DU2M / param%TU2S !! The second body of the two-body equivalent velocity vector the collider system + Mcb_si = system%cb%mass * param%MU2KG !! The central body mass of the system + select type(param) + class is (symba_parameters) + min_mfrag_si = (param%min_GMfrag / param%GU) * param%MU2KG !! The minimum fragment mass to generate. Collider systems that would otherwise generate less massive fragments than this value will be forced to merge instead + class default + min_mfrag_si = 0.0_DP + end select + + mtot = sum(mass_si(:)) + dentot = sum(mass_si(:) * density_si(:)) / mtot + + !! Use the positions and velocities of the parents from indside the step (at collision) to calculate the collisional regime + call fraggle_regime_collresolve(Mcb_si, mass_si(jtarg), mass_si(jproj), radius_si(jtarg), radius_si(jproj), x1_si(:), x2_si(:),& + v1_si(:), v2_si(:), density_si(jtarg), density_si(jproj), min_mfrag_si, frag%regime, mlr, mslr, frag%Qloss) + + frag%mass_dist(1) = min(max(mlr, 0.0_DP), mtot) + frag%mass_dist(2) = min(max(mslr, 0.0_DP), mtot) + frag%mass_dist(3) = min(max(mtot - mlr - mslr, 0.0_DP), mtot) + + ! Find the center of mass of the collisional system + frag%mtot = sum(colliders%mass(:)) + frag%xbcom(:) = (colliders%mass(1) * colliders%xb(:,1) + colliders%mass(2) * colliders%xb(:,2)) / frag%mtot + frag%vbcom(:) = (colliders%mass(1) * colliders%vb(:,1) + colliders%mass(2) * colliders%vb(:,2)) / frag%mtot + + ! Convert quantities back to the system units and save them into the fragment system + frag%mass_dist(:) = (frag%mass_dist(:) / param%MU2KG) + frag%Qloss = frag%Qloss * (param%TU2S / param%DU2M)**2 / param%MU2KG + + call fraggle_io_log_regime(colliders, frag) + end associate + + return + end subroutine fraggle_regime_colliders + + + subroutine fraggle_regime_collresolve(Mcb, m1, m2, rad1, rad2, xh1, xh2, vb1, vb2, den1, den2, min_mfrag, regime, Mlr, Mslr, Qloss) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Determine the collisional regime of two colliding bodies. + !! Current version requires all values to be converted to SI units prior to calling the function + !! References: + !! Kokubo, E., Genda, H., 2010. Formation of Terrestrial Planets from Protoplanets Under a Realistic Accretion + !! Condition. ApJL 714, L21. https://doi.org/10.1088/2041-8205/714/1/L21 + !! Leinhardt, Z.M., Stewart, S.T., 2012. Collisions between Gravity-dominated Bodies. I. Outcome Regimes and Scaling + !! Laws 745, 79. https://doi.org/10.1088/0004-637X/745/1/79 + !! Mustill, A.J., Davies, M.B., Johansen, A., 2018. The dynamical evolution of transiting planetary systems including + !! a realistic collision prescription. Mon Not R Astron Soc 478, 2896–2908. https://doi.org/10.1093/mnras/sty1273 + !! Rufu, R., Aharonson, O., 2019. Impact Dynamics of Moons Within a Planetary Potential. J. Geophys. Res. Planets 124, + !! 1008–1019. https://doi.org/10.1029/2018JE005798 + !! Stewart, S.T., Leinhardt, Z.M., 2012. Collisions between Gravity-dominated Bodies. II. The Diversity of Impact + !! Outcomes during the End Stage of Planet Formation. ApJ 751, 32. https://doi.org/10.1088/0004-637X/751/1/32 + !! + implicit none + ! Arguments + real(DP), intent(in) :: Mcb, m1, m2, rad1, rad2, den1, den2, min_mfrag + real(DP), dimension(:), intent(in) :: xh1, xh2, vb1, vb2 + integer(I4B), intent(out) :: regime + real(DP), intent(out) :: Mlr, Mslr + real(DP), intent(out) :: Qloss !! The residual energy after the collision + ! Constants + integer(I4B), parameter :: N1 = 1 !number of objects with mass equal to the largest remnant from LS12 + integer(I4B), parameter :: N2 = 2 !number of objects with mass larger than second largest remnant from LS12 + real(DP), parameter :: DENSITY1 = 1000.0_DP !standard density parameter from LS12 [kg/m3] + real(DP), parameter :: MU_BAR = 0.37_DP !0.385#0.37#0.3333# 3.978 # 1/3 material parameter for hydrodynamic planet-size bodies (LS12) + real(DP), parameter :: BETA = 2.85_DP !slope of sfd for remnants from LS12 2.85 + real(DP), parameter :: ETA = -1.50_DP !! LS12 eq. (44) + real(DP), parameter :: C1 = 2.43_DP !! Kokubo & Genda (2010) eq. (3) + real(DP), parameter :: C2 = -0.0408_DP !! Kokubo & Genda (2010) eq. (3) + real(DP), parameter :: C3 = 1.86_DP !! Kokubo & Genda (2010) eq. (3) + real(DP), parameter :: C4 = 1.08_DP !! Kokubo & Genda (2010) eq. (3) + real(DP), parameter :: CRUFU = 2.0_DP - 3 * MU_BAR ! central potential variable from Rufu and Aharonson (2019) + real(DP), parameter :: SUPERCAT_QRATIO = 1.8_DP ! See Section 4.1 of LS12 + ! Internals + real(DP) :: a1, alpha, aint, b, bcrit, c_star, egy, zeta, l, lint, mu, phi, theta + real(DP) :: Qr, Qrd_pstar, Qr_erosion, Qr_supercat + real(DP) :: Vhr, Verosion, Vescp, Vhill, Vimp, Vsupercat + real(DP) :: Mint, Mtot, Mtmp + real(DP) :: Rp, rhill + real(DP) :: Mresidual + real(DP) :: U_binding + + Vimp = norm2(vb2(:) - vb1(:)) + b = calc_b(xh2, vb2, xh1, vb1) + l = (rad1 + rad2) * (1 - b) + egy = 0.5_DP * dot_product(vb1, vb1) - GC * Mcb / norm2(xh1) + a1 = - GC * Mcb / 2.0_DP / egy + Mtot = m1 + m2 + mu = (m1 * m2) / Mtot + if (l < 2 * rad2) then + !calculate Mint + phi = 2 * acos((l - rad2) / rad2) + aint = rad2**2 * (PI - (phi - sin(phi)) / 2.0_DP) + lint = 2 * sqrt(rad2**2 - (rad2 - l / 2.0_DP) ** 2) + Mint = aint * lint ![kg] + alpha = (l**2) * (3 * rad2 - l) / (4 * (rad2**3)) + else + alpha = 1.0_DP + Mint = m2 + end if + Rp = (3 * (m1 / den1 + alpha * m2 / den2) / (4 * PI))**(1.0_DP/3.0_DP) ! (Mustill et al. 2018) + c_star = calc_c_star(Rp) + + !calculate Vescp + Vescp = sqrt(2 * GC * Mtot / Rp) !Mustill et al. 2018 eq 6 + + !calculate rhill + rhill = a1 * (m1 / 3.0_DP / (Mcb + m1))**(1.0_DP/3.0_DP) + + !calculate Vhill + if ((rad2 + rad1) < rhill) then + Vhill = sqrt(2 * GC * m1 * ((rhill**2 - rhill * (rad1 + rad2)) / & + (rhill**2 - 0.5_DP * (rad1 + rad2)**2)) / (rad1 + rad2)) + else + Vhill = Vescp + end if + + !calculate Qr_pstar + Qrd_pstar = calc_Qrd_pstar(m1, m2, alpha, c_star) * (Vhill / Vescp)**CRUFU !Rufu and Aharaonson eq (3) + + !calculate Verosion + Qr_erosion = 2 * (1.0_DP - m1 / Mtot) * Qrd_pstar + Verosion = (2 * Qr_erosion * Mtot / mu)** (1.0_DP / 2.0_DP) + Qr = mu*(Vimp**2) / Mtot / 2.0_DP + + !calculate mass largest remnant Mlr + Mlr = max((1.0_DP - Qr / Qrd_pstar / 2.0_DP) * Mtot, min_mfrag) ! [kg] # LS12 eq (5) + + !calculate Vsupercat + Qr_supercat = SUPERCAT_QRATIO * Qrd_pstar ! See LS12 Section 4.1 + Vsupercat = sqrt(2 * Qr_supercat * Mtot / mu) + + !calculate Vhr + zeta = (m1 - m2) / Mtot + theta = 1.0_DP - b + Vhr = Vescp * (C1 * zeta**2 * theta**(2.5_DP) + C2 * zeta**2 + C3 * theta**(2.5_DP) + C4) ! Kokubo & Genda (2010) eq. (3) + bcrit = rad1 / (rad1 + rad2) + Qloss = 0.0_DP + U_binding = (3.0_DP * Mtot) / (5.0_DP * Rp) ! LS12 eq. 27 + + if ((m1 < min_mfrag).or.(m2 < min_mfrag)) then + regime = COLLRESOLVE_REGIME_MERGE !perfect merging regime + Mlr = Mtot + Mslr = 0.0_DP + Qloss = 0.0_DP + call fraggle_io_log_one_message("Fragments would have mass below the minimum. Converting this collision into a merger.") + else + if( Vimp < Vescp) then + regime = COLLRESOLVE_REGIME_MERGE !perfect merging regime + Mlr = Mtot + Mslr = 0.0_DP + Qloss = 0.0_DP + else if (Vimp < Verosion) then + if (b < bcrit) then + regime = COLLRESOLVE_REGIME_MERGE !partial accretion regime" + Mlr = Mtot + Mslr = 0.0_DP + Qloss = 0.0_DP + else if ((b > bcrit) .and. (Vimp < Vhr)) then + regime = COLLRESOLVE_REGIME_MERGE ! graze and merge + Mlr = Mtot + Mslr = 0.0_DP + Qloss = 0.0_DP + else + Mlr = m1 + Mslr = max(calc_Qrd_rev(m2, m1, Mint, den1, den2, Vimp, c_star), min_mfrag) + regime = COLLRESOLVE_REGIME_HIT_AND_RUN !hit and run + Qloss = (c_star + 1.0_DP) * U_binding ! Qr + end if + else if (Vimp > Verosion .and. Vimp < Vsupercat) then + if (m2 < 0.001_DP * m1) then + regime = COLLRESOLVE_REGIME_MERGE !cratering regime" + Mlr = Mtot + Mslr = 0.0_DP + Qloss = 0.0_DP + else + Mslr = max(Mtot * (3.0_DP - BETA) * (1.0_DP - N1 * Mlr / Mtot) / (N2 * BETA), min_mfrag) ! LS12 eq (37) + regime = COLLRESOLVE_REGIME_DISRUPTION !disruption + Qloss = (c_star + 1.0_DP) * U_binding ! Qr - Qr_erosion + end if + else if (Vimp > Vsupercat) then + Mlr = max(Mtot * 0.1_DP * (Qr / (Qrd_pstar * SUPERCAT_QRATIO))**(ETA), min_mfrag) !LS12 eq (44) + Mslr = max(Mtot * (3.0_DP - BETA) * (1.0_DP - N1 * Mlr / Mtot) / (N2 * BETA), min_mfrag) !LS12 eq (37) + regime = COLLRESOLVE_REGIME_SUPERCATASTROPHIC ! supercatastrophic + Qloss = (c_star + 1.0_DP) * U_binding ! Qr - Qr_supercat + else + write(*,*) "Error no regime found in symba_regime" + end if + end if + + if (Mslr > Mlr) then ! The second-largest fragment is actually larger than the largest, so we will swap them + Mtmp = Mlr + Mlr = Mslr + Mslr = Mtmp + end if + + Mresidual = Mtot - Mlr - Mslr + if (Mresidual < 0.0_DP) then ! prevents final masses from going negative + Mlr = Mlr + Mresidual + end if + + return + + ! Internal functions + contains + function calc_Qrd_pstar(Mtarg, Mp, alpha, c_star) result(Qrd_pstar) + !! author: Jennifer L.L. Pouplin and Carlisle A. Wishard + !! + !! Calculates the corrected Q* for oblique impacts. See Eq. (15) of LS12. + !! Reference: + !! Leinhardt, Z.M., Stewart, S.T., 2012. Collisions between Gravity-dominated Bodies. I. Outcome Regimes and Scaling + !! Laws 745, 79. https://doi.org/10.1088/0004-637X/745/1/79 + !! + implicit none + ! Arguments + real(DP),intent(in) :: Mtarg, Mp, alpha, c_star + ! Result + real(DP) :: Qrd_pstar + ! Internals + real(DP) :: Qrd_star1, mu_alpha, mu, Qrd_star + + ! calc mu, mu_alpha + mu = (Mtarg * Mp) / (Mtarg + Mp) ! [kg] + mu_alpha = (Mtarg * alpha * Mp) / (Mtarg + alpha * Mp) ! [kg] + ! calc Qrd_star1 + Qrd_star1 = (c_star * 4 * PI * DENSITY1 * GC * Rp**2) / 5.0_DP + ! calc Qrd_star + Qrd_star = Qrd_star1 * (((Mp / Mtarg + 1.0_DP)**2) / (4 * Mp / Mtarg))**(2.0_DP / (3.0_DP * MU_BAR) - 1.0_DP) !(eq 23) + ! calc Qrd_pstar, v_pstar + Qrd_pstar = ((mu / mu_alpha)**(2.0_DP - 3.0_DP * MU_BAR / 2.0_DP)) * Qrd_star ! (eq 15) + + return + end function calc_Qrd_pstar + + function calc_Qrd_rev(Mp, Mtarg, Mint, den1, den2, Vimp, c_star) result(Mslr) + !! author: Jennifer L.L. Pouplin and Carlisle A. Wishard + !! + !! Calculates mass of second largest fragment. + !! + implicit none + ! Arguments + real(DP),intent(in) :: Mp, Mtarg, Mint, den1, den2, Vimp, c_star + ! Result + real(DP) :: Mslr + ! Internals + real(DP) :: mtot_rev, mu_rev, gamma_rev, Qrd_star1, Qrd_star, mu_alpha_rev + real(DP) :: Qrd_pstar, Rc1, Qr_rev, Qrd_pstar_rev, Qr_supercat_rev + + ! calc Mslr, Rc1, mu, gammalr + mtot_rev = Mint + Mp + Rc1 = (3 * (Mint / den1 + Mp / den2) / (4 * PI))**(1.0_DP/3.0_DP) ! [m] Mustill et al 2018 + mu_rev = (Mint * Mp) / mtot_rev ! [kg] eq 49 LS12 + mu_alpha_rev = (Mtarg * alpha * Mp) / (Mtarg + alpha * Mp) + gamma_rev = Mint / Mp ! eq 50 LS12 + !calc Qr_rev + Qr_rev = mu_rev * (Vimp**2) / (2 * mtot_rev) + ! calc Qrd_star1, v_star1 + Qrd_star1 = (c_star * 4 * PI * mtot_rev * GC ) / Rc1 / 5.0_DP + ! calc Qrd_pstar_rev + Qrd_star = Qrd_star1 * (((gamma_rev + 1.0_DP)**2) / (4 * gamma_rev)) ** (2.0_DP / (3.0_DP * MU_BAR) - 1.0_DP) !(eq 52) + Qrd_pstar = Qrd_star * ((mu_rev / mu_alpha_rev)**(2.0_DP - 3.0_DP * MU_BAR / 2.0_DP)) + Qrd_pstar_rev = Qrd_pstar * (Vhill / Vescp)**CRUFU !Rufu and Aharaonson eq (3) + !calc Qr_supercat_rev + Qr_supercat_rev = 1.8_DP * Qrd_pstar_rev + if (Qr_rev > Qr_supercat_rev ) then + Mslr = mtot_rev * (0.1_DP * ((Qr_rev / (Qrd_pstar_rev * 1.8_DP))**(-1.5_DP))) !eq (44) + else if ( Qr_rev < Qrd_pstar_rev ) then + Mslr = Mp + else + Mslr = (1.0_DP - Qr_rev / Qrd_pstar_rev / 2.0_DP) * (mtot_rev) ! [kg] #(eq 5) + end if + + if ( Mslr > Mp ) Mslr = Mp !check conservation of mass + + return + end function calc_Qrd_rev + + function calc_b(proj_pos, proj_vel, targ_pos, targ_vel) result(sintheta) + !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Calculates the impact factor b = sin(theta), where theta is the angle between the relative velocity + !! and distance vectors of the target and projectile bodies. See Fig. 2 of Leinhardt and Stewart (2012) + !! + implicit none + !! Arguments + real(DP), dimension(:), intent(in) :: proj_pos, proj_vel, targ_pos, targ_vel + !! Result + real(DP) :: sintheta + !! Internals + real(DP), dimension(NDIM) :: imp_vel, distance, x_cross_v + + imp_vel(:) = proj_vel(:) - targ_vel(:) + distance(:) = proj_pos(:) - targ_pos(:) + x_cross_v(:) = distance(:) .cross. imp_vel(:) + sintheta = norm2(x_cross_v(:)) / norm2(distance(:)) / norm2(imp_vel(:)) + return + end function calc_b + + + function calc_c_star(Rc1) result(c_star) + !! author: David A. Minton + !! + !! Calculates c_star as a function of impact equivalent radius. It inteRpolates between 5 for ~1 km sized bodies to + !! 1.8 for ~10000 km sized bodies. See LS12 Fig. 4 for details. + !! + implicit none + !! Arguments + real(DP), intent(in) :: Rc1 + !! Result + real(DP) :: c_star + !! Internals + real(DP), parameter :: loR = 1.0e3_DP ! Lower bound of inteRpolation size (m) + real(DP), parameter :: hiR = 1.0e7_DP ! Upper bound of inteRpolation size (m) + real(DP), parameter :: loval = 5.0_DP ! Value of C* at lower bound + real(DP), parameter :: hival = 1.9_DP ! Value of C* at upper bound + + if (Rc1 < loR) then + c_star = loval + else if (Rc1 < hiR) then + c_star = loval + (hival - loval) * log(Rc1 / loR) / log(hiR /loR) + else + c_star = hival + end if + return + end function calc_c_star + + end subroutine fraggle_regime_collresolve + +end submodule s_fraggle_regime \ No newline at end of file diff --git a/src/fraggle/fraggle_set.f90 b/src/fraggle/fraggle_set.f90 new file mode 100644 index 000000000..d520b2c5d --- /dev/null +++ b/src/fraggle/fraggle_set.f90 @@ -0,0 +1,333 @@ +submodule(fraggle_classes) s_fraggle_set + use swiftest +contains + + module subroutine fraggle_set_budgets_fragments(self, colliders) + !! author: David A. Minton + !! + !! Sets the energy and momentum budgets of the fragments based on the collider values and the before/after values of energy and momentum + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + ! Internals + real(DP) :: dEtot + real(DP), dimension(NDIM) :: dL + + associate(frag => self) + + dEtot = frag%Etot_after - frag%Etot_before + dL(:) = frag%Ltot_after(:) - frag%Ltot_before(:) + + frag%L_budget(:) = -dL(:) + frag%ke_budget = -(dEtot - 0.5_DP * frag%mtot * dot_product(frag%vbcom(:), frag%vbcom(:))) - frag%Qloss + + end associate + return + end subroutine fraggle_set_budgets_fragments + + + module subroutine fraggle_set_mass_dist_fragments(self, colliders, param) + !! author: David A. Minton + !! + !! Sets the mass of fragments based on the mass distribution returned by the regime calculation. + !! This subroutine must be run after the the setup rourtine has been run on the fragments + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + class(swiftest_parameters), intent(in) :: param !! Current Swiftest run configuration parameters + ! Internals + integer(I4B) :: i, jproj, jtarg, nfrag, istart + real(DP), dimension(2) :: volume + real(DP), dimension(NDIM) :: Ip_avg + real(DP) :: mfrag, mremaining, min_mfrag + real(DP), parameter :: BETA = 2.85_DP + integer(I4B), parameter :: NFRAGMAX = 100 !! Maximum number of fragments that can be generated + integer(I4B), parameter :: NFRAGMIN = 7 !! Minimum number of fragments that can be generated (set by the fraggle_generate algorithm for constraining momentum and energy) + integer(I4B), parameter :: NFRAG_SIZE_MULTIPLIER = 3 !! Log-space scale factor that scales the number of fragments by the collisional system mass + integer(I4B), parameter :: iMlr = 1 + integer(I4B), parameter :: iMslr = 2 + integer(I4B), parameter :: iMrem = 3 + + associate(frag => self) + ! Get mass weighted mean of Ip and density + volume(1:2) = 4._DP / 3._DP * PI * colliders%radius(1:2)**3 + Ip_avg(:) = (colliders%mass(1) * colliders%Ip(:,1) + colliders%mass(2) * colliders%Ip(:,2)) / frag%mtot + if (colliders%mass(1) > colliders%mass(2)) then + jtarg = 1 + jproj = 2 + else + jtarg = 2 + jproj = 1 + end if + + select type(param) + class is (symba_parameters) + min_mfrag = (param%min_GMfrag / param%GU) + ! The number of fragments we generate is bracked by the minimum required by fraggle_generate (7) and the + ! maximum set by the NFRAG_SIZE_MULTIPLIER which limits the total number of fragments to prevent the nbody + ! code from getting an overwhelmingly large number of fragments + nfrag = ceiling(NFRAG_SIZE_MULTIPLIER * log(frag%mtot / min_mfrag)) + nfrag = max(min(nfrag, NFRAGMAX), NFRAGMIN) + class default + min_mfrag = 0.0_DP + nfrag = NFRAGMAX + end select + + select case(frag%regime) + case(COLLRESOLVE_REGIME_DISRUPTION, COLLRESOLVE_REGIME_SUPERCATASTROPHIC, COLLRESOLVE_REGIME_HIT_AND_RUN) + ! The first two bins of the mass_dist are the largest and second-largest fragments that came out of fraggle_regime. + ! The remainder from the third bin will be distributed among nfrag-2 bodies. The following code will determine nfrag based on + ! the limits bracketed above and the model size distribution of fragments. + ! Check to see if our size distribution would give us a smaller number of fragments than the maximum number + i = iMrem + mremaining = frag%mass_dist(iMrem) + do while (i <= nfrag) + mfrag = (1 + i - iMslr)**(-3._DP / BETA) * frag%mass_dist(iMslr) + if (mremaining - mfrag < 0.0_DP) exit + mremaining = mremaining - mfrag + i = i + 1 + end do + if (i < nfrag) nfrag = max(i, NFRAGMIN) ! The sfd would actually give us fewer fragments than our maximum + + call frag%setup(nfrag, param) + case (COLLRESOLVE_REGIME_MERGE, COLLRESOLVE_REGIME_GRAZE_AND_MERGE) + call frag%setup(1, param) + frag%mass(1) = frag%mass_dist(1) + frag%radius(1) = colliders%radius(jtarg) + frag%density(1) = frag%mass_dist(1) / volume(jtarg) + frag%Ip(:, 1) = colliders%Ip(:,1) + return + case default + write(*,*) "fraggle_set_mass_dist_fragments error: Unrecognized regime code",frag%regime + end select + + ! Make the first two bins the same as the Mlr and Mslr values that came from fraggle_regime + frag%mass(1) = frag%mass_dist(iMlr) + frag%mass(2) = frag%mass_dist(iMslr) + + ! Distribute the remaining mass the 3:nfrag bodies following the model SFD given by slope BETA + mremaining = frag%mass_dist(iMrem) + do i = iMrem, nfrag + mfrag = (1 + i - iMslr)**(-3._DP / BETA) * frag%mass_dist(iMslr) + frag%mass(i) = mfrag + mremaining = mremaining - mfrag + end do + + ! If there is any residual mass (either positive or negative) we will distribute remaining mass proportionally among the the fragments + if (mremaining < 0.0_DP) then ! If the remainder is negative, this means that that the number of fragments required by the SFD is smaller than our lower limit set by fraggle_generate. + istart = iMrem ! We will reduce the mass of the 3:nfrag bodies to prevent the second-largest fragment from going smaller + else ! If the remainder is postiive, this means that the number of fragments required by the SFD is larger than our upper limit set by computational expediency. + istart = iMslr ! We will increase the mass of the 2:nfrag bodies to compensate, which ensures that the second largest fragment remains the second largest + end if + mfrag = 1._DP + mremaining / sum(frag%mass(istart:nfrag)) + frag%mass(istart:nfrag) = frag%mass(istart:nfrag) * mfrag + + ! There may still be some small residual due to round-off error. If so, simply add it to the last bin of the mass distribution. + mremaining = frag%mtot - sum(frag%mass(1:nfrag)) + frag%mass(nfrag) = frag%mass(nfrag) + mremaining + + ! Compute physical properties of the new fragments + select case(frag%regime) + case(COLLRESOLVE_REGIME_HIT_AND_RUN) ! The hit and run case always preserves the largest body intact, so there is no need to recompute the physical properties of the first fragment + frag%radius(1) = colliders%radius(jtarg) + frag%density(1) = frag%mass_dist(iMlr) / volume(jtarg) + frag%Ip(:, 1) = colliders%Ip(:,1) + istart = 2 + case default + istart = 1 + end select + frag%density(istart:nfrag) = frag%mtot / sum(volume(:)) + frag%radius(istart:nfrag) = (3 * frag%mass(istart:nfrag) / (4 * PI * frag%density(istart:nfrag)))**(1.0_DP / 3.0_DP) + do i = istart, nfrag + frag%Ip(:, i) = Ip_avg(:) + end do + + end associate + + return + end subroutine fraggle_set_mass_dist_fragments + + + module subroutine fraggle_set_coordinate_system(self, colliders) + !! author: David A. Minton + !! + !! Defines the collisional coordinate system, including the unit vectors of both the system and individual fragments. + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + ! Internals + integer(I4B) :: i + real(DP), dimension(NDIM) :: x_cross_v, delta_r, delta_v, Ltot + real(DP) :: r_col_norm, v_col_norm + real(DP), dimension(NDIM, self%nbody) :: L_sigma + + associate(frag => self, nfrag => self%nbody) + delta_v(:) = colliders%vb(:, 2) - colliders%vb(:, 1) + v_col_norm = .mag. delta_v(:) + delta_r(:) = colliders%xb(:, 2) - colliders%xb(:, 1) + r_col_norm = .mag. delta_r(:) + + ! We will initialize fragments on a plane defined by the pre-impact system, with the z-axis aligned with the angular momentum vector + ! and the y-axis aligned with the pre-impact distance vector. + Ltot = colliders%L_orbit(:,1) + colliders%L_orbit(:,2) + colliders%L_spin(:,1) + colliders%L_spin(:,2) + frag%y_coll_unit(:) = delta_r(:) / r_col_norm + frag%z_coll_unit(:) = Ltot(:) / (.mag. Ltot(:)) + ! The cross product of the y- by z-axis will give us the x-axis + frag%x_coll_unit(:) = frag%y_coll_unit(:) .cross. frag%z_coll_unit(:) + + if (.not.any(frag%x_coll(:,:) > 0.0_DP)) return + frag%rmag(:) = .mag. frag%x_coll(:,:) + + call random_number(L_sigma(:,:)) ! Randomize the tangential velocity direction. This helps to ensure that the tangential velocity doesn't completely line up with the angular momentum vector, + ! otherwise we can get an ill-conditioned system + do concurrent(i = 1:nfrag, frag%rmag(i) > 0.0_DP) + frag%v_r_unit(:, i) = frag%x_coll(:, i) / frag%rmag(i) + frag%v_n_unit(:, i) = frag%z_coll_unit(:) + 2e-1_DP * (L_sigma(:,i) - 0.5_DP) + frag%v_n_unit(:, i) = frag%v_n_unit(:, i) / (.mag. frag%v_n_unit(:, i)) + frag%v_t_unit(:, i) = frag%v_n_unit(:, i) .cross. frag%v_r_unit(:, i) + frag%v_t_unit(:, i) = frag%v_t_unit(:, i) / (.mag. frag%v_t_unit(:, i)) + end do + end associate + + return + end subroutine fraggle_set_coordinate_system + + + ! module subroutine symba_set_collresolve_colliders(self, cb, pl, idx) + ! !! author: David A. Minton + ! !! + ! !! Calculate the two-body equivalent values given a set of input collider indices + ! use swiftest_classes, only : swiftest_nbody_system + ! implicit none + ! ! Arguments + ! class(fraggle_colliders), intent(inout) :: self !! Fraggle collider object + ! class(symba_cb), intent(in) :: cb !! Swiftest central body object system object + ! class(symba_pl), intent(in) :: pl !! Swiftest central body object system object + ! integer(I4B), dimension(:), intent(in) :: idx !! Index array of bodies from the pl object to use to calculate a "two-body equivalent" collisional pair + ! ! Internals + ! real(DP), dimension(NDIM, 2) :: mxc, vc + ! real(DP), dimension(NDIM) :: vcom, xcom + + ! associate(colliders => self) + + ! ! Compute orbital angular momentum of pre-impact system + ! xcom(:) = (colliders%mass(1) * colliders%xb(:, 1) + colliders%mass(2) * colliders%xb(:, 2)) / sum(colliders%mass(:)) + ! vcom(:) = (colliders%mass(1) * colliders%vb(:, 1) + colliders%mass(2) * colliders%vb(:, 2)) / sum(colliders%mass(:)) + ! mxc(:, 1) = colliders%mass(1) * (colliders%xb(:, 1) - xcom(:)) + ! mxc(:, 2) = colliders%mass(2) * (colliders%xb(:, 2) - xcom(:)) + ! vc(:, 1) = colliders%vb(:, 1) - vcom(:) + ! vc(:, 2) = colliders%vb(:, 2) - vcom(:) + + ! colliders%L_orbit(:,:) = mxc(:,:) .cross. vc(:,:) + + ! end associate + + ! return + ! end subroutine symbe_set_collresolve_colliders + + + module subroutine fraggle_set_natural_scale_factors(self, colliders) + !! author: David A. Minton + !! + !! Scales dimenional quantities to ~O(1) with respect to the collisional system. + !! This scaling makes it easier for the non-linear minimization to converge on a solution + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + ! Internals + integer(I4B) :: i + + associate(frag => self) + ! Set scale factors + frag%Escale = 0.5_DP * (colliders%mass(1) * dot_product(colliders%vb(:,1), colliders%vb(:,1)) + colliders%mass(2) * dot_product(colliders%vb(:,2), colliders%vb(:,2))) + frag%dscale = sum(colliders%radius(:)) + frag%mscale = frag%mtot + frag%vscale = sqrt(frag%Escale / frag%mscale) + frag%tscale = frag%dscale / frag%vscale + frag%Lscale = frag%mscale * frag%dscale * frag%vscale + + ! Scale all dimensioned quantities of colliders and fragments + frag%xbcom(:) = frag%xbcom(:) / frag%dscale + frag%vbcom(:) = frag%vbcom(:) / frag%vscale + colliders%xb(:,:) = colliders%xb(:,:) / frag%dscale + colliders%vb(:,:) = colliders%vb(:,:) / frag%vscale + colliders%mass(:) = colliders%mass(:) / frag%mscale + colliders%radius(:) = colliders%radius(:) / frag%dscale + colliders%L_spin(:,:) = colliders%L_spin(:,:) / frag%Lscale + + do i = 1, 2 + colliders%rot(:,i) = colliders%L_spin(:,i) / (colliders%mass(i) * colliders%radius(i)**2 * colliders%Ip(3, i)) + end do + + frag%mtot = frag%mtot / frag%mscale + frag%mass = frag%mass / frag%mscale + frag%radius = frag%radius / frag%dscale + frag%Qloss = frag%Qloss / frag%Escale + end associate + + return + end subroutine fraggle_set_natural_scale_factors + + + module subroutine fraggle_set_original_scale_factors(self, colliders) + !! author: David A. Minton + !! + !! Restores dimenional quantities back to the system units + use, intrinsic :: ieee_exceptions + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + ! Internals + integer(I4B) :: i + logical, dimension(size(IEEE_ALL)) :: fpe_halting_modes + + call ieee_get_halting_mode(IEEE_ALL,fpe_halting_modes) ! Save the current halting modes so we can turn them off temporarily + call ieee_set_halting_mode(IEEE_ALL,.false.) + + associate(frag => self) + + ! Restore scale factors + frag%xbcom(:) = frag%xbcom(:) * frag%dscale + frag%vbcom(:) = frag%vbcom(:) * frag%vscale + + colliders%mass = colliders%mass * frag%mscale + colliders%radius = colliders%radius * frag%dscale + colliders%xb = colliders%xb * frag%dscale + colliders%vb = colliders%vb * frag%vscale + colliders%L_spin = colliders%L_spin * frag%Lscale + do i = 1, 2 + colliders%rot(:,i) = colliders%L_spin(:,i) * (colliders%mass(i) * colliders%radius(i)**2 * colliders%Ip(3, i)) + end do + frag%Qloss = frag%Qloss * frag%Escale + + frag%mtot = frag%mtot * frag%mscale + frag%mass = frag%mass * frag%mscale + frag%radius = frag%radius * frag%dscale + frag%rot = frag%rot / frag%tscale + frag%x_coll = frag%x_coll * frag%dscale + frag%v_coll = frag%v_coll * frag%vscale + + do i = 1, frag%nbody + frag%xb(:, i) = frag%x_coll(:, i) + frag%xbcom(:) + frag%vb(:, i) = frag%v_coll(:, i) + frag%vbcom(:) + end do + + frag%mscale = 1.0_DP + frag%dscale = 1.0_DP + frag%vscale = 1.0_DP + frag%tscale = 1.0_DP + frag%Lscale = 1.0_DP + frag%Escale = 1.0_DP + end associate + call ieee_set_halting_mode(IEEE_ALL,fpe_halting_modes) + + return + end subroutine fraggle_set_original_scale_factors + + +end submodule s_fraggle_set \ No newline at end of file diff --git a/src/fraggle/fraggle_setup.f90 b/src/fraggle/fraggle_setup.f90 new file mode 100644 index 000000000..65e107b03 --- /dev/null +++ b/src/fraggle/fraggle_setup.f90 @@ -0,0 +1,78 @@ +submodule (fraggle_classes) s_fraggle_setup + use swiftest +contains + + module subroutine fraggle_setup_reset_fragments(self) + !! author: David A. Minton + !! + !! Resets all position and velocity-dependent fragment quantities in order to do a fresh calculation (does not reset mass, radius, or other values that get set prior to the call to fraggle_generate) + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self + + self%xb(:,:) = 0.0_DP + self%vb(:,:) = 0.0_DP + self%rot(:,:) = 0.0_DP + self%x_coll(:,:) = 0.0_DP + self%v_coll(:,:) = 0.0_DP + self%v_r_unit(:,:) = 0.0_DP + self%v_t_unit(:,:) = 0.0_DP + self%v_n_unit(:,:) = 0.0_DP + + self%rmag(:) = 0.0_DP + self%rotmag(:) = 0.0_DP + self%v_r_mag(:) = 0.0_DP + self%v_t_mag(:) = 0.0_DP + + self%ke_orbit = 0.0_DP + self%ke_spin = 0.0_DP + self%L_orbit(:) = 0.0_DP + self%L_spin(:) = 0.0_DP + + return + end subroutine fraggle_setup_reset_fragments + + + module subroutine fraggle_setup_fragments(self, n, param) + !! author: David A. Minton + !! + !! Allocates arrays for n fragments in a Fraggle system. Passing n = 0 deallocates all arrays. + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self + integer(I4B), intent(in) :: n + class(swiftest_parameters), intent(in) :: param + + call setup_pl(self, n, param) + if (n < 0) return + + if (allocated(self%x_coll)) deallocate(self%x_coll) + if (allocated(self%v_coll)) deallocate(self%v_coll) + if (allocated(self%v_r_unit)) deallocate(self%v_r_unit) + if (allocated(self%v_t_unit)) deallocate(self%v_t_unit) + if (allocated(self%v_n_unit)) deallocate(self%v_n_unit) + if (allocated(self%rmag)) deallocate(self%rmag) + if (allocated(self%rotmag)) deallocate(self%rotmag) + if (allocated(self%v_r_mag)) deallocate(self%v_r_mag) + if (allocated(self%v_t_mag)) deallocate(self%v_t_mag) + + if (n == 0) return + + allocate(self%x_coll(NDIM,n)) + allocate(self%v_coll(NDIM,n)) + allocate(self%v_r_unit(NDIM,n)) + allocate(self%v_t_unit(NDIM,n)) + allocate(self%v_n_unit(NDIM,n)) + allocate(self%rmag(n)) + allocate(self%rotmag(n)) + allocate(self%v_r_mag(n)) + allocate(self%v_t_mag(n)) + + call self%reset() + + return + end subroutine fraggle_setup_fragments + + + +end submodule s_fraggle_setup \ No newline at end of file diff --git a/src/fraggle/fraggle_util.f90 b/src/fraggle/fraggle_util.f90 new file mode 100644 index 000000000..df8b89c41 --- /dev/null +++ b/src/fraggle/fraggle_util.f90 @@ -0,0 +1,316 @@ +submodule(fraggle_classes) s_fraggle_util + use swiftest +contains + + module subroutine fraggle_util_add_fragments_to_system(frag, colliders, system, param) + !! Author: David A. Minton + !! + !! Adds fragments to the temporary system pl object + implicit none + ! Arguments + class(fraggle_fragments), intent(in) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + ! Internals + integer(I4B) :: i, npl_before, npl_after + logical, dimension(:), allocatable :: lexclude + + associate(nfrag => frag%nbody, pl => system%pl, cb => system%cb) + npl_after = pl%nbody + npl_before = npl_after - nfrag + allocate(lexclude(npl_after)) + + pl%status(npl_before+1:npl_after) = ACTIVE + pl%mass(npl_before+1:npl_after) = frag%mass(1:nfrag) + pl%Gmass(npl_before+1:npl_after) = frag%mass(1:nfrag) * param%GU + pl%radius(npl_before+1:npl_after) = frag%radius(1:nfrag) + do concurrent (i = 1:nfrag) + pl%xb(:,npl_before+i) = frag%xb(:,i) + pl%vb(:,npl_before+i) = frag%vb(:,i) + pl%xh(:,npl_before+i) = frag%xb(:,i) - cb%xb(:) + pl%vh(:,npl_before+i) = frag%vb(:,i) - cb%vb(:) + end do + if (param%lrotation) then + pl%Ip(:,npl_before+1:npl_after) = frag%Ip(:,1:nfrag) + pl%rot(:,npl_before+1:npl_after) = frag%rot(:,1:nfrag) + end if + ! This will remove the colliders from the system since we've replaced them with fragments + lexclude(1:npl_after) = .false. + lexclude(colliders%idx(1:colliders%ncoll)) = .true. + where(lexclude(1:npl_after)) + pl%status(1:npl_after) = INACTIVE + elsewhere + pl%status(1:npl_after) = ACTIVE + endwhere + + end associate + + return + end subroutine fraggle_util_add_fragments_to_system + + + module subroutine fraggle_util_ang_mtm(self) + !! Author: David A. Minton + !! + !! Calcualtes the current angular momentum of the fragments + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + ! Internals + integer(I4B) :: i + + associate(frag => self, nfrag => self%nbody) + frag%L_orbit(:) = 0.0_DP + frag%L_spin(:) = 0.0_DP + + do i = 1, nfrag + frag%L_orbit(:) = frag%L_orbit(:) + frag%mass(i) * (frag%x_coll(:, i) .cross. frag%v_coll(:, i)) + frag%L_spin(:) = frag%L_spin(:) + frag%mass(i) * frag%radius(i)**2 * frag%Ip(:, i) * frag%rot(:, i) + end do + end associate + + return + end subroutine fraggle_util_ang_mtm + + + module subroutine fraggle_util_construct_temporary_system(frag, system, param, tmpsys, tmpparam) + !! Author: David A. Minton + !! + !! Constructs a temporary internal system consisting of active bodies and additional fragments. This internal temporary system is used to calculate system energy with and without fragments + !! and optionally including fragments. + implicit none + ! Arguments + class(fraggle_fragments), intent(in) :: frag !! Fraggle fragment system object + class(swiftest_nbody_system), intent(in) :: system !! Original swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + class(swiftest_nbody_system), allocatable, intent(out) :: tmpsys !! Output temporary swiftest nbody system object + class(swiftest_parameters), allocatable, intent(out) :: tmpparam !! Output temporary configuration run parameters + ! Internals + logical, dimension(:), allocatable :: linclude + integer(I4B) :: npl_tot + + associate(nfrag => frag%nbody, pl => system%pl, npl => system%pl%nbody, cb => system%cb) + ! Set up a new system based on the original + if (allocated(tmpparam)) deallocate(tmpparam) + if (allocated(tmpsys)) deallocate(tmpsys) + allocate(tmpparam, source=param) + call setup_construct_system(tmpsys, tmpparam) + + ! No test particles necessary for energy/momentum calcs + call tmpsys%tp%setup(0, param) + + ! Replace the empty central body object with a copy of the original + deallocate(tmpsys%cb) + allocate(tmpsys%cb, source=cb) + + ! Make space for the fragments + npl_tot = npl + nfrag + call tmpsys%pl%setup(npl_tot, tmpparam) + allocate(linclude(npl_tot)) + + ! Fill up the temporary system with all of the original bodies, leaving the spaces for fragments empty until we add them in later + linclude(1:npl) = .true. + linclude(npl+1:npl_tot) = .false. + call tmpsys%pl%fill(pl, linclude) + + ! Scale the temporary system to the natural units of the current Fraggle calculation + call tmpsys%rescale(tmpparam, frag%mscale, frag%dscale, frag%tscale) + + end associate + + return + end subroutine fraggle_util_construct_temporary_system + + + module subroutine fraggle_util_get_energy_momentum(self, colliders, system, param, lbefore) + !! Author: David A. Minton + !! + !! Calculates total system energy in either the pre-collision outcome state (lbefore = .true.) or the post-collision outcome state (lbefore = .false.) + !! This subrourtine works by building a temporary internal massive body object out of the non-excluded bodies and optionally with fragments appended. + !! This will get passed to the energy calculation subroutine so that energy is computed exactly the same way is it is in the main program. + !! This will temporarily expand the massive body object in a temporary system object called tmpsys to feed it into symba_energy + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + logical, intent(in) :: lbefore !! Flag indicating that this the "before" state of the system, with colliders included and fragments excluded or vice versa + ! Internals + integer(I4B) :: i, nplm + logical, dimension(:), allocatable :: lexclude + logical :: lk_plpl + logical, save :: ladd_frags + class(swiftest_nbody_system), allocatable, save :: tmpsys + class(swiftest_parameters), allocatable, save :: tmpparam + integer(I4B) :: npl_before, npl_after + + associate(frag => self, nfrag => self%nbody, pl => system%pl, cb => system%cb) + + ! Because we're making a copy of the massive body object with the excludes/fragments appended, we need to deallocate the + ! big k_plpl array and recreate it when we're done, otherwise we run the risk of blowing up the memory by + ! allocating two of these ginormous arrays simulteouously. This is not particularly efficient, but as this + ! subroutine should be called relatively infrequently, it shouldn't matter too much. + + npl_before = pl%nbody + npl_after = npl_before + nfrag + + ! Build the exluded body logical mask + allocate(lexclude(npl_after)) + if (lbefore) then + lexclude(1:npl_before) = .false. + lexclude(npl_before+1:npl_after) = .true. + call fraggle_util_construct_temporary_system(frag, system, param, tmpsys, tmpparam) + else + lexclude(1:npl_after) = .false. + lexclude(colliders%idx(1:colliders%ncoll)) = .true. + if (.not.allocated(tmpsys)) then + write(*,*) "Error in fraggle_util_get_energy_momentum. This must be called with lbefore=.true. at least once before calling it with lbefore=.false." + call util_exit(FAILURE) + end if + call fraggle_util_add_fragments_to_system(frag, colliders, tmpsys, tmpparam) + end if + + call tmpsys%pl%index(param) + + call tmpsys%get_energy_and_momentum(param) + + + ! Calculate the current fragment energy and momentum balances + if (lbefore) then + frag%Lorbit_before(:) = tmpsys%Lorbit(:) + frag%Lspin_before(:) = tmpsys%Lspin(:) + frag%Ltot_before(:) = tmpsys%Ltot(:) + frag%ke_orbit_before = tmpsys%ke_orbit + frag%ke_spin_before = tmpsys%ke_spin + frag%pe_before = tmpsys%pe + frag%Etot_before = tmpsys%te + else + frag%Lorbit_after(:) = tmpsys%Lorbit(:) + frag%Lspin_after(:) = tmpsys%Lspin(:) + frag%Ltot_after(:) = tmpsys%Ltot(:) + frag%ke_orbit_after = tmpsys%ke_orbit + frag%ke_spin_after = tmpsys%ke_spin + frag%pe_after = tmpsys%pe + frag%Etot_after = tmpsys%te + end if + end associate + + return + end subroutine fraggle_util_get_energy_momentum + + + module subroutine fraggle_util_restructure(self, colliders, try, f_spin, r_max_start) + !! Author: David A. Minton + !! + !! Restructure the inputs after a failed attempt failed to find a set of positions and velocities that satisfy the energy and momentum constraints + implicit none + ! Arguments + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + integer(I4B), intent(in) :: try !! The current number of times Fraggle has tried to find a solution + real(DP), intent(inout) :: f_spin !! Fraction of energy/momentum that goes into spin. This decreases ater a failed attempt + real(DP), intent(inout) :: r_max_start !! The maximum radial distance that the position calculation starts with. This increases after a failed attempt + ! Internals + integer(I4B) :: i + real(DP), save :: ke_tot_deficit, r_max_start_old, ke_avg_deficit_old + real(DP), dimension(:), allocatable :: m_frag_new, rad_frag_new + real(DP), dimension(:,:), allocatable :: xb_frag_new, vb_frag_new, Ip_frag_new, rot_frag_new + real(DP) :: delta_r, delta_r_max, ke_avg_deficit + real(DP), parameter :: ke_avg_deficit_target = 0.0_DP + + ! Introduce a bit of noise in the radius determination so we don't just flip flop between similar failed positions + associate(frag => self) + call random_number(delta_r_max) + delta_r_max = sum(colliders%radius(:)) * (1.0_DP + 2e-1_DP * (delta_r_max - 0.5_DP)) + if (try == 1) then + ke_tot_deficit = - (frag%ke_budget - frag%ke_orbit - frag%ke_spin) + ke_avg_deficit = ke_tot_deficit + delta_r = delta_r_max + else + ! Linearly interpolate the last two failed solution ke deficits to find a new distance value to try + ke_tot_deficit = ke_tot_deficit - (frag%ke_budget - frag%ke_orbit - frag%ke_spin) + ke_avg_deficit = ke_tot_deficit / try + delta_r = (r_max_start - r_max_start_old) * (ke_avg_deficit_target - ke_avg_deficit_old) / (ke_avg_deficit - ke_avg_deficit_old) + if (abs(delta_r) > delta_r_max) delta_r = sign(delta_r_max, delta_r) + end if + r_max_start_old = r_max_start + r_max_start = r_max_start + delta_r ! The larger lever arm can help if the problem is in the angular momentum step + ke_avg_deficit_old = ke_avg_deficit + + if (f_spin > epsilon(1.0_DP)) then ! Try reducing the fraction in spin + f_spin = f_spin / 2 + else + f_spin = 0.0_DP + end if + end associate + + return + end subroutine fraggle_util_restructure + + + module subroutine fraggle_util_shift_vector_to_origin(m_frag, vec_frag) + !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Adjusts the position or velocity of the fragments as needed to align them with the origin + implicit none + ! Arguments + real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses + real(DP), dimension(:,:), intent(inout) :: vec_frag !! Fragment positions or velocities in the center of mass frame + + ! Internals + real(DP), dimension(NDIM) :: mvec_frag, COM_offset + integer(I4B) :: i, nfrag + real(DP) :: mtot + + mvec_frag(:) = 0.0_DP + mtot = sum(m_frag) + nfrag = size(m_frag) + + do i = 1, nfrag + mvec_frag = mvec_frag(:) + vec_frag(:,i) * m_frag(i) + end do + COM_offset(:) = -mvec_frag(:) / mtot + do i = 1, nfrag + vec_frag(:, i) = vec_frag(:, i) + COM_offset(:) + end do + + return + end subroutine fraggle_util_shift_vector_to_origin + + + module function fraggle_util_vmag_to_vb(v_r_mag, v_r_unit, v_t_mag, v_t_unit, m_frag, vcom) result(vb) + !! Author: David A. Minton + !! + !! Converts radial and tangential velocity magnitudes into barycentric velocity + implicit none + ! Arguments + real(DP), dimension(:), intent(in) :: v_r_mag !! Unknown radial component of fragment velocity vector + real(DP), dimension(:), intent(in) :: v_t_mag !! Tangential component of velocity vector set previously by angular momentum constraint + real(DP), dimension(:,:), intent(in) :: v_r_unit, v_t_unit !! Radial and tangential unit vectors for each fragment + real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses + real(DP), dimension(:), intent(in) :: vcom !! Barycentric velocity of collisional system center of mass + ! Result + real(DP), dimension(:,:), allocatable :: vb + ! Internals + integer(I4B) :: i, nfrag + + allocate(vb, mold=v_r_unit) + ! Make sure the velocity magnitude stays positive + nfrag = size(m_frag) + do i = 1, nfrag + vb(:,i) = abs(v_r_mag(i)) * v_r_unit(:, i) + end do + ! In order to keep satisfying the kinetic energy constraint, we must shift the origin of the radial component of the velocities to the center of mass + call fraggle_util_shift_vector_to_origin(m_frag, vb) + + do i = 1, nfrag + vb(:, i) = vb(:, i) + v_t_mag(i) * v_t_unit(:, i) + vcom(:) + end do + + return + end function fraggle_util_vmag_to_vb + + +end submodule s_fraggle_util diff --git a/src/fragmentation/fragmentation.f90 b/src/fragmentation/fragmentation.f90 deleted file mode 100644 index 73cef6240..000000000 --- a/src/fragmentation/fragmentation.f90 +++ /dev/null @@ -1,1178 +0,0 @@ -submodule(swiftest_classes) s_fragmentation - use swiftest -contains - - module subroutine fragmentation_initialize(system, param, family, x, v, L_spin, Ip, mass, radius, & - nfrag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, Qloss, lfailure) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Initialize the position and velocity of fragments to conserve energy and momentum. - use, intrinsic :: ieee_exceptions - implicit none - ! Arguments - class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - integer(I4B), dimension(:), intent(in) :: family !! Index of bodies involved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Two-body equivalent position, vector, spin momentum, and rotational inertia values for the collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Two-body equivalent mass and radii for the bodies in the collision - integer(I4B), intent(inout) :: nfrag !! Number of fragments to generate - real(DP), dimension(:), allocatable, intent(inout) :: m_frag, rad_frag !! Distribution of fragment mass and radii - real(DP), dimension(:,:), allocatable, intent(inout) :: Ip_frag !! Fragment rotational inertia vectors - real(DP), dimension(:,:), allocatable, intent(inout) :: xb_frag, vb_frag, rot_frag !! Fragment barycentric position, barycentric velocity, and rotation vectors - real(DP), intent(inout) :: Qloss !! Energy lost during the collision - logical, intent(out) :: lfailure !! Answers the question: Should this have been a merger instead? - ! Internals - real(DP) :: mscale, dscale, vscale, tscale, Lscale, Escale ! Scale factors that reduce quantities to O(~1) in the collisional system - real(DP) :: mtot - real(DP), dimension(NDIM) :: xcom, vcom - integer(I4B) :: ii, npl_new - logical, dimension(:), allocatable :: lexclude - real(DP), dimension(NDIM, 2) :: rot, L_orb - real(DP), dimension(:,:), allocatable :: x_frag, v_frag, v_r_unit, v_t_unit, v_h_unit - real(DP), dimension(:), allocatable :: rmag, rotmag, v_r_mag, v_t_mag - real(DP), dimension(NDIM) :: Ltot_before - real(DP), dimension(NDIM) :: Ltot_after - real(DP) :: Etot_before, ke_orbit_before, ke_spin_before, pe_before, Lmag_before - real(DP) :: Etot_after, ke_orbit_after, ke_spin_after, pe_after, Lmag_after, dEtot, dLmag - real(DP), dimension(NDIM) :: L_frag_tot, L_frag_orb - real(DP) :: ke_frag_budget, ke_frag_orbit, ke_radial, ke_frag_spin, ke_avg_deficit, ke_avg_deficit_old - real(DP), dimension(NDIM) :: x_col_unit, y_col_unit, z_col_unit - character(len=*), parameter :: fmtlabel = "(A14,10(ES11.4,1X,:))" - integer(I4B) :: try, subtry - integer(I4B), parameter :: NFRAG_MIN = 7 !! The minimum allowable number of fragments (set to 6 because that's how many unknowns are needed in the tangential velocity calculation) - real(DP) :: r_max_start, r_max_start_old, r_max, f_spin - real(DP), parameter :: Ltol = 10 * epsilon(1.0_DP) - real(DP), parameter :: Etol = 1e-9_DP - integer(I4B), parameter :: MAXTRY = 3000 - integer(I4B), parameter :: TANTRY = 3 - logical, dimension(size(IEEE_ALL)) :: fpe_halting_modes, fpe_quiet_modes - class(swiftest_nbody_system), allocatable :: tmpsys - class(swiftest_parameters), allocatable :: tmpparam - - if (nfrag < NFRAG_MIN) then - write(*,*) "symba_frag_pos needs at least ",NFRAG_MIN," fragments, but only ",nfrag," were given." - lfailure = .true. - return - end if - - call ieee_get_halting_mode(IEEE_ALL,fpe_halting_modes) ! Save the current halting modes so we can turn them off temporarily - fpe_quiet_modes(:) = .false. - call ieee_set_halting_mode(IEEE_ALL,fpe_quiet_modes) - - f_spin = 0.05_DP - - allocate(x_frag, source=xb_frag) - allocate(v_frag, source=vb_frag) - - associate(pl => system%pl, npl => system%pl%nbody) - npl_new = npl + nfrag - allocate(lexclude(npl_new)) - lexclude(1:npl) = pl%status(1:npl) == INACTIVE - lexclude(npl+1:npl_new) = .true. - end associate - - call set_scale_factors() - call define_coordinate_system() - call construct_temporary_system() - - ! Calculate the initial energy of the system without the collisional family - call calculate_system_energy(linclude_fragments=.false.) - - r_max_start = norm2(x(:,2) - x(:,1)) - try = 1 - lfailure = .false. - ke_avg_deficit = 0.0_DP - do while (try < MAXTRY) - lfailure = .false. - ke_avg_deficit_old = ke_avg_deficit - ke_avg_deficit = 0.0_DP - subtry = 1 - do - ! Initialize the fragments with 0 velocity and spin so we can divide up the balance between the tangential, radial, and spin components while conserving momentum - xb_frag(:,:) = 0.0_DP - vb_frag(:,:) = 0.0_DP - rot_frag(:,:) = 0.0_DP - v_t_mag(:) = 0.0_DP - v_r_mag(:) = 0.0_DP - call set_fragment_position_vectors() - call calculate_system_energy(linclude_fragments=.true.) - ke_frag_budget = -dEtot - Qloss - call set_fragment_tan_vel(lfailure) - ke_avg_deficit = ke_avg_deficit - ke_radial - subtry = subtry + 1 - if (.not.lfailure .or. subtry == TANTRY) exit - !write(*,*) 'Trying new arrangement' - end do - ke_avg_deficit = ke_avg_deficit / subtry - !if (lfailure) write(*,*) 'Failed to find tangential velocities' - - if (.not.lfailure) then - call calculate_system_energy(linclude_fragments=.true.) - ke_radial = -dEtot - Qloss - call set_fragment_radial_velocities(lfailure) - ! if (lfailure) write(*,*) 'Failed to find radial velocities' - if (.not.lfailure) then - call calculate_system_energy(linclude_fragments=.true.) - ! write(*,*) 'Qloss : ',Qloss - ! write(*,*) '-dEtot: ',-dEtot - ! write(*,*) 'delta : ',abs((dEtot + Qloss)) - if ((abs(dEtot + Qloss) > Etol) .or. (dEtot > 0.0_DP)) then - !write(*,*) 'Failed due to high energy error: ',dEtot, abs(dEtot + Qloss) / Etol - lfailure = .true. - else if (abs(dLmag) / Lmag_before > Ltol) then - !write(*,*) 'Failed due to high angular momentum error: ', dLmag / Lmag_before - lfailure = .true. - end if - end if - end if - - if (.not.lfailure) exit - call restructure_failed_fragments() - try = try + 1 - end do - call restore_scale_factors() - call calculate_system_energy(linclude_fragments=.true.) - - ! write(*, "(' -------------------------------------------------------------------------------------')") - ! write(*, "(' Final diagnostic')") - ! write(*, "(' -------------------------------------------------------------------------------------')") - ! if (lfailure) then - ! write(*,*) "symba_frag_pos failed after: ",try," tries" - ! do ii = 1, nfrag - ! vb_frag(:, ii) = vcom(:) - ! end do - ! else - ! write(*,*) "symba_frag_pos succeeded after: ",try," tries" - ! write(*, "(' dL_tot should be very small' )") - ! write(*,fmtlabel) ' dL_tot |', dLmag / Lmag_before - ! write(*, "(' dE_tot should be negative and equal to Qloss' )") - ! write(*,fmtlabel) ' dE_tot |', dEtot / abs(Etot_before) - ! write(*,fmtlabel) ' Qloss |', -Qloss / abs(Etot_before) - ! write(*,fmtlabel) ' dE - Qloss |', (Etot_after - Etot_before + Qloss) / abs(Etot_before) - ! end if - ! write(*, "(' -------------------------------------------------------------------------------------')") - - call ieee_set_halting_mode(IEEE_ALL,fpe_halting_modes) ! Save the current halting modes so we can turn them off temporarily - - return - - contains - - ! Because of the complexity of this procedure, we have chosen to break it up into a series of nested subroutines. - subroutine set_scale_factors() - !! author: David A. Minton - !! - !! Scales dimenional quantities to ~O(1) with respect to the collisional system. This scaling makes it easier for the non-linear minimization - !! to converge on a solution - implicit none - integer(I4B) :: i - - ! Find the center of mass of the collisional system - mtot = sum(mass(:)) - xcom(:) = (mass(1) * x(:,1) + mass(2) * x(:,2)) / mtot - vcom(:) = (mass(1) * v(:,1) + mass(2) * v(:,2)) / mtot - - ! Set scale factors - dscale = sum(radius(:)) - mscale = mtot - vscale = (mass(1) * norm2(v(:,1) - vcom(:)) + mass(2) * norm2(v(:,2) - vcom(:))) / mtot - tscale = dscale / vscale - Lscale = mscale * dscale * vscale - Escale = mscale * vscale**2 - - xcom(:) = xcom(:) / dscale - vcom(:) = vcom(:) / vscale - - mtot = mtot / mscale - mass = mass / mscale - radius = radius / dscale - x = x / dscale - v = v / vscale - L_spin = L_spin / Lscale - do i = 1, 2 - rot(:,i) = L_spin(:,i) / (mass(i) * radius(i)**2 * Ip(3, i)) - end do - - m_frag = m_frag / mscale - rad_frag = rad_frag / dscale - Qloss = Qloss / Escale - - return - end subroutine set_scale_factors - - - subroutine restore_scale_factors() - !! author: David A. Minton - !! - !! Restores dimenional quantities back to the system units - implicit none - integer(I4B) :: i - - call ieee_set_halting_mode(IEEE_ALL,.false.) - ! Restore scale factors - xcom(:) = xcom(:) * dscale - vcom(:) = vcom(:) * vscale - - mtot = mtot * mscale - mass = mass * mscale - radius = radius * dscale - x = x * dscale - v = v * vscale - L_spin = L_spin * Lscale - do i = 1, 2 - rot(:,i) = L_spin(:,i) * (mass(i) * radius(i)**2 * Ip(3, i)) - end do - - m_frag = m_frag * mscale - rad_frag = rad_frag * dscale - rot_frag = rot_frag / tscale - x_frag = x_frag * dscale - v_frag = v_frag * vscale - Qloss = Qloss * Escale - - do i = 1, nfrag - xb_frag(:, i) = x_frag(:, i) + xcom(:) - vb_frag(:, i) = v_frag(:, i) + vcom(:) - end do - - Etot_before = Etot_before * Escale - pe_before = pe_before * Escale - ke_spin_before = ke_spin_before * Escale - ke_orbit_before = ke_orbit_before * Escale - Ltot_before = Ltot_before * Lscale - Lmag_before = Lmag_before * Lscale - Etot_after = Etot_after * Escale - pe_after = pe_after * Escale - ke_spin_after = ke_spin_after * Escale - ke_orbit_after = ke_orbit_after * Escale - Ltot_after = Ltot_after * Lscale - Lmag_after = Lmag_after * Lscale - - dLmag = norm2(Ltot_after(:) - Ltot_before(:)) - dEtot = Etot_after - Etot_before - - call tmpsys%rescale(tmpparam, mscale**(-1), dscale**(-1), tscale**(-1)) - - mscale = 1.0_DP - dscale = 1.0_DP - vscale = 1.0_DP - tscale = 1.0_DP - Lscale = 1.0_DP - Escale = 1.0_DP - - return - end subroutine restore_scale_factors - - - subroutine define_coordinate_system() - !! author: David A. Minton - !! - !! Defines the collisional coordinate system, including the unit vectors of both the system and individual fragments. - implicit none - integer(I4B) :: i - real(DP), dimension(NDIM) :: x_cross_v, xc, vc, delta_r, delta_v - real(DP) :: r_col_norm, v_col_norm - - allocate(rmag(nfrag)) - allocate(rotmag(nfrag)) - allocate(v_r_mag(nfrag)) - allocate(v_t_mag(nfrag)) - allocate(v_r_unit(NDIM,nfrag)) - allocate(v_t_unit(NDIM,nfrag)) - allocate(v_h_unit(NDIM,nfrag)) - - rmag(:) = 0.0_DP - rotmag(:) = 0.0_DP - v_r_mag(:) = 0.0_DP - v_t_mag(:) = 0.0_DP - v_r_unit(:,:) = 0.0_DP - v_t_unit(:,:) = 0.0_DP - v_h_unit(:,:) = 0.0_DP - - L_orb(:, :) = 0.0_DP - ! Compute orbital angular momentum of pre-impact system - do i = 1, 2 - xc(:) = x(:, i) - xcom(:) - vc(:) = v(:, i) - vcom(:) - x_cross_v(:) = xc(:) .cross. vc(:) - L_orb(:, i) = mass(i) * x_cross_v(:) - end do - - ! Compute orbital angular momentum of pre-impact system. This will be the normal vector to the collision fragment plane - L_frag_tot(:) = L_spin(:, 1) + L_spin(:, 2) + L_orb(:, 1) + L_orb(:, 2) - - delta_v(:) = v(:, 2) - v(:, 1) - v_col_norm = norm2(delta_v(:)) - delta_r(:) = x(:, 2) - x(:, 1) - r_col_norm = norm2(delta_r(:)) - - ! We will initialize fragments on a plane defined by the pre-impact system, with the z-axis aligned with the angular momentum vector - ! and the y-axis aligned with the pre-impact distance vector. - y_col_unit(:) = delta_r(:) / r_col_norm - z_col_unit(:) = L_frag_tot(:) / norm2(L_frag_tot) - ! The cross product of the y- by z-axis will give us the x-axis - x_col_unit(:) = y_col_unit(:) .cross. z_col_unit(:) - - return - end subroutine define_coordinate_system - - - subroutine construct_temporary_system() - !! Author: David A. Minton - !! - !! Constructs a temporary internal system consisting of active bodies and additional fragments. This internal temporary system is used to calculate system energy with and without fragments - !! and optionally including fragments. - implicit none - ! Internals - logical, dimension(:), allocatable :: lexclude_tmp - - associate(pl => system%pl, npl => system%pl%nbody, cb => system%cb) - if (size(lexclude) /= npl + nfrag) then - allocate(lexclude_tmp(npl_new)) - lexclude_tmp(1:npl) = lexclude(1:npl) - call move_alloc(lexclude_tmp, lexclude) - end if - where (pl%status(1:npl) == INACTIVE) ! Safety check in case one of the included bodies has been previously deactivated - lexclude(1:npl) = .true. - elsewhere - lexclude(1:npl) = .false. - end where - lexclude(npl+1:npl_new) = .true. - if (allocated(tmpparam)) deallocate(tmpparam) - allocate(tmpparam, source=param) - call setup_construct_system(tmpsys, param) - call tmpsys%tp%setup(0, param) - deallocate(tmpsys%cb) - allocate(tmpsys%cb, source=cb) - call tmpsys%pl%setup(npl + nfrag, tmpparam) - call tmpsys%pl%fill(pl, .not.lexclude) - call tmpsys%rescale(tmpparam, mscale, dscale, tscale) - - end associate - - return - end subroutine construct_temporary_system - - - subroutine add_fragments_to_tmpsys() - !! Author: David A. Minton - !! - !! Adds fragments to the temporary system pl object - implicit none - ! Internals - integer(I4B) :: i - - associate(pl => system%pl, npl => system%pl%nbody) - - tmpsys%pl%mass(npl+1:npl_new) = m_frag(1:nfrag) - tmpsys%pl%Gmass(npl+1:npl_new) = m_frag(1:nfrag) * tmpparam%GU - tmpsys%pl%radius(npl+1:npl_new) = rad_frag(1:nfrag) - do concurrent (i = 1:nfrag) - tmpsys%pl%xb(:,npl+i) = xb_frag(:,i) - tmpsys%pl%vb(:,npl+i) = vb_frag(:,i) - tmpsys%pl%xh(:,npl+i) = xb_frag(:,i) - tmpsys%cb%xb(:) - tmpsys%pl%vh(:,npl+i) = vb_frag(:,i) - tmpsys%cb%vb(:) - end do - if (tmpparam%lrotation) then - tmpsys%pl%Ip(:,npl+1:npl_new) = Ip_frag(:,1:nfrag) - tmpsys%pl%rot(:,npl+1:npl_new) = rot_frag(:,1:nfrag) - end if - ! Disable the collisional family for subsequent energy calculations and coordinate shifts - lexclude(family(:)) = .true. - lexclude(npl+1:npl_new) = .false. - where(lexclude(:)) - tmpsys%pl%status(:) = INACTIVE - elsewhere - tmpsys%pl%status(:) = ACTIVE - end where - - end associate - - return - end subroutine add_fragments_to_tmpsys - - - subroutine calculate_system_energy(linclude_fragments) - !! Author: David A. Minton - !! - !! Calculates total system energy, including all bodies in the pl list that do not have a corresponding value of the lexclude array that is true - !! and optionally including fragments. - implicit none - ! Arguments - logical, intent(in) :: linclude_fragments - ! Internals - integer(I4B) :: i, nplm - logical, dimension(:), allocatable :: lexclude_tmp - logical :: lk_plpl - - ! Because we're making a copy of symba_pl with the excludes/fragments appended, we need to deallocate the - ! big k_plpl array and recreate it when we're done, otherwise we run the risk of blowing up the memory by - ! allocating two of these ginormous arrays simulteouously. This is not particularly efficient, but as this - ! subroutine should be called relatively infrequently, it shouldn't matter too much. - - ! Build the internal planet list out of the non-excluded bodies and optionally with fragments appended. This - ! will get passed to the energy calculation subroutine so that energy is computed exactly the same way is it - ! is in the main program. This will temporarily expand the planet list in a temporary system object called tmpsys to feed it into symba_energy - associate(pl => system%pl, npl => system%pl%nbody, cb => system%cb) - - where (lexclude(1:npl_new)) - tmpsys%pl%status(1:npl_new) = INACTIVE - elsewhere - tmpsys%pl%status(1:npl_new) = ACTIVE - end where - - select type(plwksp => tmpsys%pl) - class is (symba_pl) - select type(param) - class is (symba_parameters) - plwksp%nplm = count(plwksp%Gmass > param%Gmtiny / mscale) - end select - end select - - lk_plpl = allocated(pl%k_plpl) - if (lk_plpl) deallocate(pl%k_plpl) - - call tmpsys%pl%eucl_index() - - call tmpsys%get_energy_and_momentum(param) - - ! Restore the big array - deallocate(tmpsys%pl%k_plpl) - select type(pl) - class is (symba_pl) - select type(param) - class is (symba_parameters) - pl%nplm = count(pl%Gmass > param%Gmtiny) - end select - end select - - if (lk_plpl) call pl%eucl_index() - - ! Calculate the current fragment energy and momentum balances - if (linclude_fragments) then - Ltot_after(:) = tmpsys%Lorbit(:) + tmpsys%Lspin(:) - Lmag_after = norm2(Ltot_after(:)) - ke_orbit_after = tmpsys%ke_orbit - ke_spin_after = tmpsys%ke_spin - pe_after = tmpsys%pe - Etot_after = ke_orbit_after + ke_spin_after + pe_after - dEtot = Etot_after - Etot_before - dLmag = norm2(Ltot_after(:) - Ltot_before(:)) - else - Ltot_before(:) = tmpsys%Lorbit(:) + tmpsys%Lspin(:) - Lmag_before = norm2(Ltot_before(:)) - ke_orbit_before = tmpsys%ke_orbit - ke_spin_before = tmpsys%ke_spin - pe_before = tmpsys%pe - Etot_before = ke_orbit_before + ke_spin_before + pe_before - end if - end associate - - return - end subroutine calculate_system_energy - - - subroutine shift_vector_to_origin(m_frag, vec_frag) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Adjusts the position or velocity of the fragments as needed to align them with the origin - implicit none - ! Arguments - real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses - real(DP), dimension(:,:), intent(inout) :: vec_frag !! Fragment positions or velocities in the center of mass frame - - ! Internals - real(DP), dimension(NDIM) :: mvec_frag, COM_offset - integer(I4B) :: i - - mvec_frag(:) = 0.0_DP - - do i = 1, nfrag - mvec_frag = mvec_frag(:) + vec_frag(:,i) * m_frag(i) - end do - COM_offset(:) = -mvec_frag(:) / mtot - do i = 1, nfrag - vec_frag(:, i) = vec_frag(:, i) + COM_offset(:) - end do - - return - end subroutine shift_vector_to_origin - - - subroutine set_fragment_position_vectors() - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Initializes the orbits of the fragments around the center of mass. The fragments are initially placed on a plane defined by the - !! pre-impact angular momentum. They are distributed on an ellipse surrounding the center of mass. - !! The initial positions do not conserve energy or momentum, so these need to be adjusted later. - - implicit none - real(DP) :: dis, rad - real(DP), dimension(NDIM) :: L_sigma - logical, dimension(:), allocatable :: loverlap - integer(I4B) :: i, j - - allocate(loverlap(nfrag)) - - ! Place the fragments into a region that is big enough that we should usually not have overlapping bodies - ! An overlapping bodies will collide in the next time step, so it's not a major problem if they do (it just slows the run down) - r_max = r_max_start - rad = sum(radius(:)) - - ! We will treat the first two fragments of the list as special cases. They get initialized the maximum distances apart along the original impactor distance vector. - ! This is done because in a regular disruption, the first body is the largest, the second the second largest, and the rest are smaller equal-mass fragments. - - call random_number(x_frag(:,3:nfrag)) - loverlap(:) = .true. - do while (any(loverlap(3:nfrag))) - x_frag(:, 1) = x(:, 1) - xcom(:) - x_frag(:, 2) = x(:, 2) - xcom(:) - r_max = r_max + 0.1_DP * rad - do i = 3, nfrag - if (loverlap(i)) then - call random_number(x_frag(:,i)) - x_frag(:, i) = 2 * (x_frag(:, i) - 0.5_DP) * r_max - end if - end do - loverlap(:) = .false. - do j = 1, nfrag - do i = j + 1, nfrag - dis = norm2(x_frag(:,j) - x_frag(:,i)) - loverlap(i) = loverlap(i) .or. (dis <= (rad_frag(i) + rad_frag(j))) - end do - end do - end do - call shift_vector_to_origin(m_frag, x_frag) - - do i = 1, nfrag - rmag(i) = norm2(x_frag(:, i)) - v_r_unit(:, i) = x_frag(:, i) / rmag(i) - call random_number(L_sigma(:)) ! Randomize the tangential velocity direction. This helps to ensure that the tangential velocity doesn't completely line up with the angular momentum vector, - ! otherwise we can get an ill-conditioned system - v_h_unit(:, i) = z_col_unit(:) + 2e-1_DP * (L_sigma(:) - 0.5_DP) - v_h_unit(:, i) = v_h_unit(:, i) / norm2(v_h_unit(:, i)) - v_t_unit(:, i) = v_h_unit(:, i) .cross. v_r_unit(:, i) - xb_frag(:,i) = x_frag(:,i) + xcom(:) - end do - - call add_fragments_to_tmpsys() - - xcom(:) = 0.0_DP - do i = 1, nfrag - xcom(:) = xcom(:) + m_frag(i) * xb_frag(:,i) - end do - xcom(:) = xcom(:) / mtot - - return - end subroutine set_fragment_position_vectors - - - subroutine set_fragment_tan_vel(lerr) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Adjusts the tangential velocities and spins of a collection of fragments such that they conserve angular momentum without blowing the fragment kinetic energy budget. - !! This procedure works in several stages, with a goal to solve the angular and linear momentum constraints on the fragments, while still leaving a positive balance of - !! our fragment kinetic energy (ke_frag_budget) that we can put into the radial velocity distribution. - !! - !! The first thing we'll try to do is solve for the tangential velocities of the first 6 fragments, using angular and linear momentum as constraints and an initial - !! tangential velocity distribution for the remaining bodies (if there are any) that distributes their angular momentum equally between them. - !! If that doesn't work and we blow our kinetic energy budget, we will attempt to find a tangential velocity distribution that minimizes the kinetic energy while - !! conserving momentum. - !! - !! A failure will trigger a restructuring of the fragments so we will try new values of the radial position distribution. - implicit none - ! Arguments - logical, intent(out) :: lerr - ! Internals - integer(I4B) :: i - real(DP), parameter :: TOL = 1e-4_DP - real(DP), dimension(:), allocatable :: v_t_initial - real(DP), dimension(nfrag) :: kefrag - type(lambda_obj) :: spinfunc - type(lambda_obj_err) :: objective_function - real(DP), dimension(NDIM) :: L_frag_spin, L_remainder, Li, rot_L, rot_ke - - lerr = .false. - - if (ke_frag_budget < 0.0_DP) then - write(*,*) 'Negative ke_frag_budget: ',ke_frag_budget - r_max_start = r_max_start / 2 - lerr = .true. - return - end if - - allocate(v_t_initial, mold=v_t_mag) - - L_frag_spin(:) = 0.0_DP - ke_frag_spin = 0.0_DP - ! Start the first two bodies with the same rotation as the original two impactors, then distribute the remaining angular momentum among the rest - do i = 1, 2 - rot_frag(:, i) = rot(:, i) - L_frag_spin(:) = L_frag_spin(:) + m_frag(i) * rad_frag(i)**2 * Ip_frag(3, i) * rot_frag(:, i) - end do - L_frag_orb(:) = L_frag_tot(:) - L_frag_spin(:) - L_frag_spin(:) = 0.0_DP - do i = 1, nfrag - ! Convert a fraction (f_spin) of either the remaining angular momentum or kinetic energy budget into spin, whichever gives the smaller rotation so as not to blow any budgets - rot_ke(:) = sqrt(2 * f_spin * ke_frag_budget / (nfrag * m_frag(i) * rad_frag(i)**2 * Ip_frag(3, i))) * L_frag_orb(:) / norm2(L_frag_orb(:)) - rot_L(:) = f_spin * L_frag_orb(:) / (nfrag * m_frag(i) * rad_frag(i)**2 * Ip_frag(3, i)) - if (norm2(rot_ke) < norm2(rot_L)) then - rot_frag(:,i) = rot_frag(:, i) + rot_ke(:) - else - rot_frag(:, i) = rot_frag(:, i) + rot_L(:) - end if - L_frag_spin(:) = L_frag_spin(:) + m_frag(i) * rad_frag(i)**2 * Ip_frag(3, i) * rot_frag(:, i) - ke_frag_spin = ke_frag_spin + m_frag(i) * Ip_frag(3, i) * rad_frag(i)**2 * dot_product(rot_frag(:, i), rot_frag(:, i)) - end do - ke_frag_spin = 0.5_DP * ke_frag_spin - ! Convert a fraction of the pre-impact angular momentum into fragment spin angular momentum - L_frag_orb(:) = L_frag_tot(:) - L_frag_spin(:) - L_remainder(:) = L_frag_orb(:) - ! Next we will solve for the tangential component of the velocities that both conserves linear momentum and uses the remaining angular momentum not used in spin. - ! This will be done using a linear solver that solves for the tangential velocities of the first 6 fragments, constrained by the linear and angular momentum vectors, - ! which is embedded in a non-linear minimizer that will adjust the tangential velocities of the remaining i>6 fragments to minimize kinetic energy for a given momentum solution - ! The initial conditions fed to the minimizer for the fragments will be the remaining angular momentum distributed between the fragments. - do i = 1, nfrag - v_t_initial(i) = norm2(L_remainder(:)) / ((nfrag - i + 1) * m_frag(i) * norm2(x_frag(:,i))) - Li(:) = m_frag(i) * x_frag(:,i) .cross. v_t_initial(i) * v_t_unit(:, i) - L_remainder(:) = L_remainder(:) - Li(:) - end do - - ! Find the local kinetic energy minimum for the system that conserves linear and angular momentum - objective_function = lambda_obj(tangential_objective_function, lerr) - v_t_mag(7:nfrag) = util_minimize_bfgs(objective_function, nfrag-6, v_t_initial(7:nfrag), TOL, lerr) - ! Now that the KE-minimized values of the i>6 fragments are found, calculate the momentum-conserving solution for tangential velociteis - v_t_initial(7:nfrag) = v_t_mag(7:nfrag) - v_t_mag(1:nfrag) = solve_fragment_tan_vel(v_t_mag_input=v_t_initial(7:nfrag), lerr=lerr) - - ! Perform one final shift of the radial velocity vectors to align with the center of mass of the collisional system (the origin) - vb_frag(:,1:nfrag) = vmag_to_vb(v_r_mag(1:nfrag), v_r_unit(:,1:nfrag), v_t_mag(1:nfrag), v_t_unit(:,1:nfrag), m_frag(1:nfrag), vcom(:)) - call add_fragments_to_tmpsys() - - ! Now do a kinetic energy budget check to make sure we are still within the budget. - kefrag = 0.0_DP - do concurrent(i = 1:nfrag) - v_frag(:, i) = vb_frag(:, i) - vcom(:) - kefrag(i) = m_frag(i) * dot_product(vb_frag(:, i), vb_frag(:, i)) - end do - ke_frag_orbit = 0.5_DP * sum(kefrag(:)) - ke_radial = ke_frag_budget - ke_frag_orbit - ke_frag_spin - - ! If we are over the energy budget, flag this as a failure so we can try again - lerr = (ke_radial < 0.0_DP) - ! write(*,*) 'Tangential' - ! write(*,*) 'Failure? ',lerr - ! write(*,*) 'ke_frag_budget: ',ke_frag_budget - ! write(*,*) 'ke_frag_spin : ',ke_frag_spin - ! write(*,*) 'ke_tangential : ',ke_frag_orbit - ! write(*,*) 'ke_remainder : ',ke_radial - - return - end subroutine set_fragment_tan_vel - - - function tangential_objective_function(v_t_mag_input, lerr) result(fval) - !! Author: David A. Minton - !! - !! Objective function for evaluating how close our fragment velocities get to minimizing KE error from our required value - implicit none - ! Arguments - real(DP), dimension(:), intent(in) :: v_t_mag_input !! Unknown tangential component of velocity vector set previously by angular momentum constraint - logical, intent(out) :: lerr !! Error flag - ! Result - real(DP) :: fval - ! Internals - integer(I4B) :: i - real(DP), dimension(NDIM,nfrag) :: v_shift - real(DP), dimension(nfrag) :: v_t_new, kearr - real(DP) :: keo - - lerr = .false. - - v_t_new(:) = solve_fragment_tan_vel(v_t_mag_input=v_t_mag_input(:), lerr=lerr) - v_shift(:,:) = vmag_to_vb(v_r_mag, v_r_unit, v_t_new, v_t_unit, m_frag, vcom) - - kearr = 0.0_DP - do concurrent(i = 1:nfrag) - kearr(i) = m_frag(i) * dot_product(v_shift(:, i), v_shift(:, i)) - end do - keo = 0.5_DP * sum(kearr(:)) - fval = keo - lerr = .false. - - return - end function tangential_objective_function - - - function solve_fragment_tan_vel(lerr, v_t_mag_input) result(v_t_mag_output) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Adjusts the positions, velocities, and spins of a collection of fragments such that they conserve angular momentum - implicit none - ! Arguments - logical, intent(out) :: lerr !! Error flag - real(DP), dimension(:), optional, intent(in) :: v_t_mag_input !! Unknown tangential velocities for fragments 7:nfrag - ! Internals - integer(I4B) :: i - ! Result - real(DP), dimension(:), allocatable :: v_t_mag_output - - real(DP), dimension(2 * NDIM, 2 * NDIM) :: A ! LHS of linear equation used to solve for momentum constraint in Gauss elimination code - real(DP), dimension(2 * NDIM) :: b ! RHS of linear equation used to solve for momentum constraint in Gauss elimination code - real(DP), dimension(NDIM) :: L_lin_others, L_orb_others, L, vtmp - - v_frag(:,:) = 0.0_DP - lerr = .false. - - ! We have 6 constraint equations (2 vector constraints in 3 dimensions each) - ! The first 3 are that the linear momentum of the fragments is zero with respect to the collisional barycenter - ! The second 3 are that the sum of the angular momentum of the fragments is conserved from the pre-impact state - L_lin_others(:) = 0.0_DP - L_orb_others(:) = 0.0_DP - do i = 1, nfrag - if (i <= 2 * NDIM) then ! The tangential velocities of the first set of bodies will be the unknowns we will solve for to satisfy the constraints - A(1:3, i) = m_frag(i) * v_t_unit(:, i) - L(:) = v_r_unit(:, i) .cross. v_t_unit(:, i) - A(4:6, i) = m_frag(i) * rmag(i) * L(:) - else if (present(v_t_mag_input)) then - vtmp(:) = v_t_mag_input(i - 6) * v_t_unit(:, i) - L_lin_others(:) = L_lin_others(:) + m_frag(i) * vtmp(:) - L(:) = x_frag(:, i) .cross. vtmp(:) - L_orb_others(:) = L_orb_others(:) + m_frag(i) * L(:) - end if - end do - b(1:3) = -L_lin_others(:) - b(4:6) = L_frag_orb(:) - L_orb_others(:) - allocate(v_t_mag_output(nfrag)) - v_t_mag_output(1:6) = util_solve_linear_system(A, b, 6, lerr) - if (present(v_t_mag_input)) v_t_mag_output(7:nfrag) = v_t_mag_input(:) - - return - end function solve_fragment_tan_vel - - - subroutine set_fragment_radial_velocities(lerr) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! - !! Adjust the fragment velocities to set the fragment orbital kinetic energy. This will minimize the difference between the fragment kinetic energy and the energy budget - implicit none - ! Arguments - logical, intent(out) :: lerr - ! Internals - real(DP), parameter :: TOL = 1e-10_DP - integer(I4B) :: i, j - real(DP), dimension(:), allocatable :: v_r_initial, v_r_sigma - real(DP), dimension(:,:), allocatable :: v_r - real(DP), dimension(nfrag) :: kearr, kespinarr - type(lambda_obj) :: objective_function - - ! Set the "target" ke_orbit_after (the value of the orbital kinetic energy that the fragments ought to have) - - allocate(v_r_initial, source=v_r_mag) - ! Initialize radial velocity magnitudes with a random value that is approximately 10% of that found by distributing the kinetic energy equally - allocate(v_r_sigma, source=v_r_mag) - call random_number(v_r_sigma(1:nfrag)) - v_r_sigma(1:nfrag) = sqrt(1.0_DP + 2 * (v_r_sigma(1:nfrag) - 0.5_DP) * 1e-4_DP) - v_r_initial(1:nfrag) = v_r_sigma(1:nfrag) * sqrt(abs(2 * ke_radial) / (m_frag(1:nfrag) * nfrag)) - - ! Initialize the lambda function using a structure constructor that calls the init method - ! Minimize the ke objective function using the BFGS optimizer - objective_function = lambda_obj(radial_objective_function) - v_r_mag = util_minimize_bfgs(objective_function, nfrag, v_r_initial, TOL, lerr) - ! Shift the radial velocity vectors to align with the center of mass of the collisional system (the origin) - vb_frag(:,1:nfrag) = vmag_to_vb(v_r_mag(1:nfrag), v_r_unit(:,1:nfrag), v_t_mag(1:nfrag), v_t_unit(:,1:nfrag), m_frag(1:nfrag), vcom(:)) - do i = 1, nfrag - v_frag(:, i) = vb_frag(:, i) - vcom(:) - end do - call add_fragments_to_tmpsys() - - do concurrent(i = 1:nfrag) - kearr(i) = m_frag(i) * dot_product(vb_frag(:, i), vb_frag(:, i)) - kespinarr(i) = m_frag(i) * Ip_frag(3, i) * rad_frag(i)**2 * dot_product(rot_frag(:,i), rot_frag(:,i)) - end do - ke_frag_orbit = 0.5_DP * sum(kearr(:)) - ke_frag_spin = 0.5_DP * sum(kespinarr(:)) - ! write(*,*) 'Radial' - ! write(*,*) 'Failure? ',lerr - ! write(*,*) 'ke_frag_budget: ',ke_frag_budget - ! write(*,*) 'ke_frag_spin : ',ke_frag_spin - ! write(*,*) 'ke_frag_orbit : ',ke_frag_orbit - ! write(*,*) 'ke_remainder : ',ke_frag_budget - (ke_frag_orbit + ke_frag_spin) - lerr = .false. - - return - end subroutine set_fragment_radial_velocities - - - function radial_objective_function(v_r_mag_input) result(fval) - !! Author: David A. Minton - !! - !! Objective function for evaluating how close our fragment velocities get to minimizing KE error from our required value - implicit none - ! Arguments - real(DP), dimension(:), intent(in) :: v_r_mag_input !! Unknown radial component of fragment velocity vector - ! Result - real(DP) :: fval !! The objective function result, which is the square of the difference between the calculated fragment kinetic energy and our target - !! Minimizing this brings us closer to our objective - ! Internals - integer(I4B) :: i - real(DP), dimension(:,:), allocatable :: v_shift - real(DP), dimension(nfrag) :: kearr - real(DP) :: keo - - allocate(v_shift, mold=vb_frag) - v_shift(:,:) = vmag_to_vb(v_r_mag_input, v_r_unit, v_t_mag, v_t_unit, m_frag, vcom) - do concurrent(i = 1:nfrag) - kearr(i) = m_frag(i) * (Ip_frag(3, i) * rad_frag(i)**2 * dot_product(rot_frag(:, i), rot_frag(:, i)) + dot_product(v_shift(:, i), v_shift(:, i))) - end do - keo = 2 * ke_frag_budget - sum(kearr(:)) - ! The following ensures that fval = 0 is a local minimum, which is what the BFGS method is searching for - fval = (keo / (2 * ke_radial))**2 - - return - end function radial_objective_function - - - function vmag_to_vb(v_r_mag, v_r_unit, v_t_mag, v_t_unit, m_frag, vcom) result(vb) - !! Author: David A. Minton - !! - !! Converts radial and tangential velocity magnitudes into barycentric velocity - implicit none - ! Arguments - real(DP), dimension(:), intent(in) :: v_r_mag !! Unknown radial component of fragment velocity vector - real(DP), dimension(:), intent(in) :: v_t_mag !! Tangential component of velocity vector set previously by angular momentum constraint - real(DP), dimension(:,:), intent(in) :: v_r_unit, v_t_unit !! Radial and tangential unit vectors for each fragment - real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses - real(DP), dimension(:), intent(in) :: vcom !! Barycentric velocity of collisional system center of mass - ! Result - real(DP), dimension(:,:), allocatable :: vb - ! Internals - integer(I4B) :: i - - allocate(vb, mold=v_r_unit) - ! Make sure the velocity magnitude stays positive - do i = 1, nfrag - vb(:,i) = abs(v_r_mag(i)) * v_r_unit(:, i) - end do - ! In order to keep satisfying the kinetic energy constraint, we must shift the origin of the radial component of the velocities to the center of mass - call shift_vector_to_origin(m_frag, vb) - - do i = 1, nfrag - vb(:, i) = vb(:, i) + v_t_mag(i) * v_t_unit(:, i) + vcom(:) - end do - - return - end function vmag_to_vb - - - subroutine restructure_failed_fragments() - !! Author: David A. Minton - !! - !! We failed to find a set of positions and velocities that satisfy all the constraints, and so we will alter the fragments and try again. - implicit none - integer(I4B) :: i - real(DP), dimension(:), allocatable :: m_frag_new, rad_frag_new - real(DP), dimension(:,:), allocatable :: xb_frag_new, vb_frag_new, Ip_frag_new, rot_frag_new - real(DP) :: delta_r, delta_r_max - real(DP), parameter :: ke_avg_deficit_target = 0.0_DP - - ! Introduce a bit of noise in the radius determination so we don't just flip flop between similar failed positions - call random_number(delta_r_max) - delta_r_max = sum(radius(:)) * (1.0_DP + 2e-1_DP * (delta_r_max - 0.5_DP)) - if (try > 2) then - ! Linearly interpolate the last two failed solution ke deficits to find a new distance value to try - delta_r = (r_max_start - r_max_start_old) * (ke_avg_deficit_target - ke_avg_deficit_old) / (ke_avg_deficit - ke_avg_deficit_old) - if (abs(delta_r) > delta_r_max) delta_r = sign(delta_r_max, delta_r) - else - delta_r = delta_r_max - end if - r_max_start_old = r_max_start - r_max_start = r_max_start + delta_r ! The larger lever arm can help if the problem is in the angular momentum step - if (f_spin > epsilon(1.0_DP)) then - f_spin = f_spin / 2 - else - f_spin = 0.0_DP - end if - - return - end subroutine restructure_failed_fragments - end subroutine fragmentation_initialize - - - module subroutine fragmentation_regime(Mcb, m1, m2, rad1, rad2, xh1, xh2, vb1, vb2, den1, den2, regime, Mlr, Mslr, mtiny, Qloss) - !! Author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Determine the collisional regime of two colliding bodies. - !! Current version requires all values to be converted to SI units prior to calling the function - !! References: - !! Kokubo, E., Genda, H., 2010. Formation of Terrestrial Planets from Protoplanets Under a Realistic Accretion - !! Condition. ApJL 714, L21. https://doi.org/10.1088/2041-8205/714/1/L21 - !! Leinhardt, Z.M., Stewart, S.T., 2012. Collisions between Gravity-dominated Bodies. I. Outcome Regimes and Scaling - !! Laws 745, 79. https://doi.org/10.1088/0004-637X/745/1/79 - !! Mustill, A.J., Davies, M.B., Johansen, A., 2018. The dynamical evolution of transiting planetary systems including - !! a realistic collision prescription. Mon Not R Astron Soc 478, 2896–2908. https://doi.org/10.1093/mnras/sty1273 - !! Rufu, R., Aharonson, O., 2019. Impact Dynamics of Moons Within a Planetary Potential. J. Geophys. Res. Planets 124, - !! 1008–1019. https://doi.org/10.1029/2018JE005798 - !! Stewart, S.T., Leinhardt, Z.M., 2012. Collisions between Gravity-dominated Bodies. II. The Diversity of Impact - !! Outcomes during the End Stage of Planet Formation. ApJ 751, 32. https://doi.org/10.1088/0004-637X/751/1/32 - !! - implicit none - ! Arguments - integer(I4B), intent(out) :: regime - real(DP), intent(out) :: Mlr, Mslr - real(DP), intent(in) :: Mcb, m1, m2, rad1, rad2, den1, den2, mtiny - real(DP), dimension(:), intent(in) :: xh1, xh2, vb1, vb2 - real(DP), intent(out) :: Qloss !! The residual energy after the collision - ! Constants - integer(I4B), parameter :: N1 = 1 !number of objects with mass equal to the largest remnant from LS12 - integer(I4B), parameter :: N2 = 2 !number of objects with mass larger than second largest remnant from LS12 - real(DP), parameter :: DENSITY1 = 1000.0_DP !standard density parameter from LS12 [kg/m3] - real(DP), parameter :: MU_BAR = 0.37_DP !0.385#0.37#0.3333# 3.978 # 1/3 material parameter for hydrodynamic planet-size bodies (LS12) - real(DP), parameter :: BETA = 2.85_DP !slope of sfd for remnants from LS12 2.85 - real(DP), parameter :: C1 = 2.43_DP !! Kokubo & Genda (2010) eq. (3) - real(DP), parameter :: C2 = -0.0408_DP !! Kokubo & Genda (2010) eq. (3) - real(DP), parameter :: C3 = 1.86_DP !! Kokubo & Genda (2010) eq. (3) - real(DP), parameter :: C4 = 1.08_DP !! Kokubo & Genda (2010) eq. (3) - real(DP), parameter :: CRUFU = 2.0_DP - 3 * MU_BAR ! central potential variable from Rufu and Aharonson (2019) - real(DP), parameter :: SUPERCAT_QRATIO = 1.8_DP ! See Section 4.1 of LS12 - ! Internals - real(DP) :: a1, alpha, aint, b, bcrit, c_star, egy, zeta, l, lint, mu, phi, theta - real(DP) :: Qr, Qrd_pstar, Qr_erosion, Qr_supercat - real(DP) :: Vhr, Verosion, Vescp, Vhill, Vimp, Vsupercat - real(DP) :: Mint, Mtot - real(DP) :: Rp, rhill - real(DP) :: Mresidual - real(DP) :: U_binding - - Vimp = norm2(vb2(:) - vb1(:)) - b = calc_b(xh2, vb2, xh1, vb1) - l = (rad1 + rad2) * (1 - b) - egy = 0.5_DP * dot_product(vb1, vb1) - GC * Mcb / norm2(xh1) - a1 = - GC * Mcb / 2.0_DP / egy - Mtot = m1 + m2 - mu = (m1 * m2) / Mtot - if (l < 2 * rad2) then - !calculate Mint - phi = 2 * acos((l - rad2) / rad2) - aint = rad2**2 * (PI - (phi - sin(phi)) / 2.0_DP) - lint = 2 * sqrt(rad2**2 - (rad2 - l / 2.0_DP) ** 2) - Mint = aint * lint ![kg] - alpha = (l**2) * (3 * rad2 - l) / (4 * (rad2**3)) - else - alpha = 1.0_DP - Mint = m2 - end if - Rp = (3 * (m1 / den1 + alpha * m2 / den2) / (4 * PI))**(1.0_DP/3.0_DP) ! (Mustill et al. 2018) - c_star = calc_c_star(Rp) - !calculate Vescp - Vescp = sqrt(2 * GC * Mtot / Rp) !Mustill et al. 2018 eq 6 - !calculate rhill - rhill = a1 * (m1 / 3.0_DP / (Mcb + m1))**(1.0_DP/3.0_DP) - !calculate Vhill - if ((rad2 + rad1) < rhill) then - Vhill = sqrt(2 * GC * m1 * ((rhill**2 - rhill * (rad1 + rad2)) / & - (rhill**2 - 0.5_DP * (rad1 + rad2)**2)) / (rad1 + rad2)) - else - Vhill = Vescp - end if - !calculate Qr_pstar - Qrd_pstar = calc_Qrd_pstar(m1, m2, alpha, c_star) * (Vhill / Vescp)**CRUFU !Rufu and Aharaonson eq (3) - !calculate Verosion - Qr_erosion = 2 * (1.0_DP - m1 / Mtot) * Qrd_pstar - Verosion = (2 * Qr_erosion * Mtot / mu)** (1.0_DP / 2.0_DP) - Qr = mu*(Vimp**2) / Mtot / 2.0_DP - !calculate mass largest remnant Mlr - Mlr = (1.0_DP - Qr / Qrd_pstar / 2.0_DP) * Mtot ! [kg] # LS12 eq (5) - !calculate Vsupercat - Qr_supercat = SUPERCAT_QRATIO * Qrd_pstar ! See LS12 Section 4.1 - Vsupercat = sqrt(2 * Qr_supercat * Mtot / mu) - !calculate Vhr - zeta = (m1 - m2) / Mtot - theta = 1.0_DP - b - Vhr = Vescp * (C1 * zeta**2 * theta**(2.5_DP) + C2 * zeta**2 + C3 * theta**(2.5_DP) + C4) ! Kokubo & Genda (2010) eq. (3) - bcrit = rad1 / (rad1 + rad2) - Qloss = 0.0_DP - U_binding = (3.0_DP * Mtot) / (5.0_DP * Rp) ! LS12 eq. 27 - - if ((m1 < mtiny).or.(m2 < mtiny)) then - regime = COLLRESOLVE_REGIME_MERGE !perfect merging regime - Mlr = Mtot - Mslr = 0.0_DP - Qloss = 0.0_DP - write(*,*) "FORCE MERGE" - else - if( Vimp < Vescp) then - regime = COLLRESOLVE_REGIME_MERGE !perfect merging regime - Mlr = Mtot - Mslr = 0.0_DP - Qloss = 0.0_DP - else if (Vimp < Verosion) then - if (b < bcrit) then - regime = COLLRESOLVE_REGIME_MERGE !partial accretion regime" - Mlr = Mtot - Mslr = 0.0_DP - Qloss = 0.0_DP - else if ((b > bcrit) .and. (Vimp < Vhr)) then - regime = COLLRESOLVE_REGIME_MERGE ! graze and merge - Mlr = Mtot - Mslr = 0.0_DP - Qloss = 0.0_DP - else - Mlr = m1 - Mslr = calc_Qrd_rev(m2, m1, Mint, den1, den2, Vimp, c_star) - regime = COLLRESOLVE_REGIME_HIT_AND_RUN !hit and run - Qloss = (c_star + 1.0_DP) * U_binding ! Qr - end if - else if (Vimp > Verosion .and. Vimp < Vsupercat) then - if (m2 < 0.001_DP * m1) then - regime = COLLRESOLVE_REGIME_MERGE !cratering regime" - Mlr = Mtot - Mslr = 0.0_DP - Qloss = 0.0_DP - else - Mslr = Mtot * (3.0_DP - BETA) * (1.0_DP - N1 * Mlr / Mtot) / (N2 * BETA) ! LS12 eq (37) - regime = COLLRESOLVE_REGIME_DISRUPTION !disruption - Qloss = (c_star + 1.0_DP) * U_binding ! Qr - Qr_erosion - end if - else if (Vimp > Vsupercat) then - Mlr = Mtot * 0.1_DP * (Qr / (Qrd_pstar * SUPERCAT_QRATIO))**(-1.5_DP) !LS12 eq (44) - Mslr = Mtot * (3.0_DP - BETA) * (1.0_DP - N1 * Mlr / Mtot) / (N2 * BETA) !LS12 eq (37) - regime = COLLRESOLVE_REGIME_SUPERCATASTROPHIC ! supercatastrophic - Qloss = (c_star + 1.0_DP) * U_binding ! Qr - Qr_supercat - else - write(*,*) "Error no regime found in symba_regime" - end if - end if - Mresidual = Mtot - Mlr - Mslr - if (Mresidual < 0.0_DP) then ! prevents final masses from going negative - Mlr = Mlr + Mresidual - end if - - return - - ! Internal functions - contains - function calc_Qrd_pstar(Mtarg, Mp, alpha, c_star) result(Qrd_pstar) - !! author: Jennifer L.L. Pouplin and Carlisle A. Wishard - !! - !! Calculates the corrected Q* for oblique impacts. See Eq. (15) of LS12. - !! Reference: - !! Leinhardt, Z.M., Stewart, S.T., 2012. Collisions between Gravity-dominated Bodies. I. Outcome Regimes and Scaling - !! Laws 745, 79. https://doi.org/10.1088/0004-637X/745/1/79 - !! - implicit none - ! Arguments - real(DP),intent(in) :: Mtarg, Mp, alpha, c_star - ! Result - real(DP) :: Qrd_pstar - ! Internals - real(DP) :: Qrd_star1, mu_alpha, mu, Qrd_star - - ! calc mu, mu_alpha - mu = (Mtarg * Mp) / (Mtarg + Mp) ! [kg] - mu_alpha = (Mtarg * alpha * Mp) / (Mtarg + alpha * Mp) ! [kg] - ! calc Qrd_star1 - Qrd_star1 = (c_star * 4 * PI * DENSITY1 * GC * Rp**2) / 5.0_DP - ! calc Qrd_star - Qrd_star = Qrd_star1 * (((Mp / Mtarg + 1.0_DP)**2) / (4 * Mp / Mtarg))**(2.0_DP / (3.0_DP * MU_BAR) - 1.0_DP) !(eq 23) - ! calc Qrd_pstar, v_pstar - Qrd_pstar = ((mu / mu_alpha)**(2.0_DP - 3.0_DP * MU_BAR / 2.0_DP)) * Qrd_star ! (eq 15) - - return - end function calc_Qrd_pstar - - function calc_Qrd_rev(Mp, Mtarg, Mint, den1, den2, Vimp, c_star) result(Mslr) - !! author: Jennifer L.L. Pouplin and Carlisle A. Wishard - !! - !! Calculates mass of second largest fragment. - !! - implicit none - ! Arguments - real(DP),intent(in) :: Mp, Mtarg, Mint, den1, den2, Vimp, c_star - ! Result - real(DP) :: Mslr - ! Internals - real(DP) :: mtot_rev, mu_rev, gamma_rev, Qrd_star1, Qrd_star, mu_alpha_rev - real(DP) :: Qrd_pstar, Rc1, Qr_rev, Qrd_pstar_rev, Qr_supercat_rev - - ! calc Mslr, Rc1, mu, gammalr - mtot_rev = Mint + Mp - Rc1 = (3 * (Mint / den1 + Mp / den2) / (4 * PI))**(1.0_DP/3.0_DP) ! [m] Mustill et al 2018 - mu_rev = (Mint * Mp) / mtot_rev ! [kg] eq 49 LS12 - mu_alpha_rev = (Mtarg * alpha * Mp) / (Mtarg + alpha * Mp) - gamma_rev = Mint / Mp ! eq 50 LS12 - !calc Qr_rev - Qr_rev = mu_rev * (Vimp**2) / (2 * mtot_rev) - ! calc Qrd_star1, v_star1 - Qrd_star1 = (c_star * 4 * PI * mtot_rev * GC ) / Rc1 / 5.0_DP - ! calc Qrd_pstar_rev - Qrd_star = Qrd_star1 * (((gamma_rev + 1.0_DP)**2) / (4 * gamma_rev)) ** (2.0_DP / (3.0_DP * MU_BAR) - 1.0_DP) !(eq 52) - Qrd_pstar = Qrd_star * ((mu_rev / mu_alpha_rev)**(2.0_DP - 3.0_DP * MU_BAR / 2.0_DP)) - Qrd_pstar_rev = Qrd_pstar * (Vhill / Vescp)**CRUFU !Rufu and Aharaonson eq (3) - !calc Qr_supercat_rev - Qr_supercat_rev = 1.8_DP * Qrd_pstar_rev - if (Qr_rev > Qr_supercat_rev ) then - Mslr = mtot_rev * (0.1_DP * ((Qr_rev / (Qrd_pstar_rev * 1.8_DP))**(-1.5_DP))) !eq (44) - else if ( Qr_rev < Qrd_pstar_rev ) then - Mslr = Mp - else - Mslr = (1.0_DP - Qr_rev / Qrd_pstar_rev / 2.0_DP) * (mtot_rev) ! [kg] #(eq 5) - end if - - if ( Mslr > Mp ) Mslr = Mp !check conservation of mass - - return - end function calc_Qrd_rev - - function calc_b(proj_pos, proj_vel, targ_pos, targ_vel) result(sintheta) - !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Calculates the impact factor b = sin(theta), where theta is the angle between the relative velocity - !! and distance vectors of the target and projectile bodies. See Fig. 2 of Leinhardt and Stewart (2012) - !! - implicit none - !! Arguments - real(DP), dimension(:), intent(in) :: proj_pos, proj_vel, targ_pos, targ_vel - !! Result - real(DP) :: sintheta - !! Internals - real(DP), dimension(NDIM) :: imp_vel, distance, x_cross_v - - imp_vel(:) = proj_vel(:) - targ_vel(:) - distance(:) = proj_pos(:) - targ_pos(:) - x_cross_v(:) = distance(:) .cross. imp_vel(:) - sintheta = norm2(x_cross_v(:)) / norm2(distance(:)) / norm2(imp_vel(:)) - return - end function calc_b - - function calc_c_star(Rc1) result(c_star) - !! author: David A. Minton - !! - !! Calculates c_star as a function of impact equivalent radius. It inteRpolates between 5 for ~1 km sized bodies to - !! 1.8 for ~10000 km sized bodies. See LS12 Fig. 4 for details. - !! - implicit none - !! Arguments - real(DP), intent(in) :: Rc1 - !! Result - real(DP) :: c_star - !! Internals - real(DP), parameter :: loR = 1.0e3_DP ! Lower bound of inteRpolation size (m) - real(DP), parameter :: hiR = 1.0e7_DP ! Upper bound of inteRpolation size (m) - real(DP), parameter :: loval = 5.0_DP ! Value of C* at lower bound - real(DP), parameter :: hival = 1.9_DP ! Value of C* at upper bound - - if (Rc1 < loR) then - c_star = loval - else if (Rc1 < hiR) then - c_star = loval + (hival - loval) * log(Rc1 / loR) / log(hiR /loR) - else - c_star = hival - end if - return - end function calc_c_star - - end subroutine fragmentation_regime - -end submodule s_fragmentation \ No newline at end of file diff --git a/src/helio/helio_coord.f90 b/src/helio/helio_coord.f90 deleted file mode 100644 index f40781810..000000000 --- a/src/helio/helio_coord.f90 +++ /dev/null @@ -1,113 +0,0 @@ -submodule (helio_classes) s_helio_coord - use swiftest -contains - - module subroutine helio_coord_vb2vh_pl(self, cb) - !! author: David A. Minton - !! - !! Convert massive bodies from barycentric to heliocentric coordinates (velocity only) - !! - !! Adapted from David E. Kaufmann's Swifter routine coord_vb2vh.f90 - !! Adapted from Hal Levison's Swift routine coord_vb2vh.f - implicit none - ! Arguments - class(helio_pl), intent(inout) :: self !! Helio massive body object - class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - ! Internals - integer(I4B) :: i - - if (self%nbody == 0) return - - associate(pl => self, npl => self%nbody) - do i = 1, NDIM - cb%vb(i) = -sum(pl%Gmass(1:npl) * pl%vb(i, 1:npl)) / cb%Gmass - pl%vh(i, 1:npl) = pl%vb(i, 1:npl) - cb%vb(i) - end do - end associate - - return - end subroutine helio_coord_vb2vh_pl - - - module subroutine helio_coord_vb2vh_tp(self, vbcb) - !! author: David A. Minton - !! - !! Convert test particles from barycentric to heliocentric coordinates (velocity only) - !! - !! Adapted from David E. Kaufmann's Swifter routine coord_vb2vh_tp.f90 - !! Adapted from Hal Levison's Swift routine coord_vb2h_tp.f - implicit none - ! Arguments - class(helio_tp), intent(inout) :: self !! Helio massive body object - real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body - - if (self%nbody == 0) return - - associate(tp => self, ntp => self%nbody) - where (tp%lmask(1:ntp)) - tp%vh(1, 1:ntp) = tp%vb(1, 1:ntp) - vbcb(1) - tp%vh(2, 1:ntp) = tp%vb(2, 1:ntp) - vbcb(2) - tp%vh(3, 1:ntp) = tp%vb(3, 1:ntp) - vbcb(3) - end where - end associate - - return - end subroutine helio_coord_vb2vh_tp - - - module subroutine helio_coord_vh2vb_pl(self, cb) - !! author: David A. Minton - !! - !! Convert massive bodies from heliocentric to barycentric coordinates (velocity only) - !! - !! Adapted from David E. Kaufmann's Swifter routine coord_vh2vb.f90 - !! Adapted from Hal Levison's Swift routine coord_vh2b.f - implicit none - ! Arguments - class(helio_pl), intent(inout) :: self !! Helio massive body object - class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - ! Internals - integer(I4B) :: i - real(DP) :: Gmtot - - if (self%nbody == 0) return - - associate(pl => self, npl => self%nbody) - Gmtot = cb%Gmass + sum(pl%Gmass(1:npl)) - do i = 1, NDIM - cb%vb(i) = -sum(pl%Gmass(1:npl) * pl%vh(i, 1:npl)) / Gmtot - pl%vb(i, 1:npl) = pl%vh(i, 1:npl) + cb%vb(i) - end do - end associate - - return - end subroutine helio_coord_vh2vb_pl - - - module subroutine helio_coord_vh2vb_tp(self, vbcb) - !! author: David A. Minton - !! - !! Convert test particles from heliocentric to barycentric coordinates (velocity only) - !! - !! Adapted from David E. Kaufmann's Swifter routine coord_vh2vb_tp.f90 - !! Adapted from Hal Levison's Swift routine coord_vh2b_tp.f - implicit none - ! Arguments - class(helio_tp), intent(inout) :: self !! Helio massive body object - real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body - - if (self%nbody == 0) return - - associate(tp => self, ntp => self%nbody) - where (tp%lmask(1:ntp)) - tp%vb(1, 1:ntp) = tp%vh(1, 1:ntp) + vbcb(1) - tp%vb(2, 1:ntp) = tp%vh(2, 1:ntp) + vbcb(2) - tp%vb(3, 1:ntp) = tp%vh(3, 1:ntp) + vbcb(3) - end where - end associate - - return - end subroutine helio_coord_vh2vb_tp - -end submodule s_helio_coord - diff --git a/src/helio/helio_kick.f90 b/src/helio/helio_kick.f90 index eebd17f53..8e7571a0b 100644 --- a/src/helio/helio_kick.f90 +++ b/src/helio/helio_kick.f90 @@ -65,9 +65,9 @@ module subroutine helio_kick_getacch_tp(self, system, param, t, lbeg) associate(tp => self, cb => system%cb, pl => system%pl, npl => system%pl%nbody) system%lbeg = lbeg if (system%lbeg) then - call tp%accel_int(pl%Gmass(:), pl%xbeg(:,:), npl) + call tp%accel_int(pl%Gmass(1:npl), pl%xbeg(:,1:npl), npl) else - call tp%accel_int(pl%Gmass(:), pl%xend(:,:), npl) + call tp%accel_int(pl%Gmass(1:npl), pl%xend(:,1:npl), npl) end if if (param%loblatecb) call tp%accel_obl(system) if (param%lextra_force) call tp%accel_user(system, param, t, lbeg) @@ -99,7 +99,7 @@ module subroutine helio_kick_vb_pl(self, system, param, t, dt, lbeg) if (self%nbody == 0) return associate(pl => self, npl => self%nbody) - pl%ah(:,:) = 0.0_DP + pl%ah(:, 1:npl) = 0.0_DP call pl%accel(system, param, t, lbeg) if (lbeg) then call pl%set_beg_end(xbeg = pl%xh) @@ -136,7 +136,7 @@ module subroutine helio_kick_vb_tp(self, system, param, t, dt, lbeg) if (self%nbody == 0) return associate(tp => self, ntp => self%nbody) - tp%ah(:,:) = 0.0_DP + tp%ah(:, 1:ntp) = 0.0_DP call tp%accel(system, param, t, lbeg) do concurrent(i = 1:ntp, tp%lmask(i)) tp%vb(:, i) = tp%vb(:, i) + tp%ah(:, i) * dt diff --git a/src/helio/helio_setup.f90 b/src/helio/helio_setup.f90 new file mode 100644 index 000000000..cf5f57d8a --- /dev/null +++ b/src/helio/helio_setup.f90 @@ -0,0 +1,24 @@ +submodule(helio_classes) s_helio_setup + use swiftest +contains + + module subroutine helio_setup_initialize_system(self, param) + !! author: David A. Minton + !! + !! Initialize a Helio nbody system from files, converting all heliocentric quantities to barycentric. + !! + implicit none + ! Arguments + class(helio_nbody_system), intent(inout) :: self !! Helio nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + + call whm_setup_initialize_system(self, param) + call self%pl%h2b(self%cb) + call self%tp%h2b(self%cb) + call self%pl%sort("mass", ascending=.false.) + call self%pl%index(param) + + return + end subroutine helio_setup_initialize_system + +end submodule s_helio_setup \ No newline at end of file diff --git a/src/io/io.f90 b/src/io/io.f90 index 2fa42dcc1..eacaacf48 100644 --- a/src/io/io.f90 +++ b/src/io/io.f90 @@ -13,12 +13,11 @@ module subroutine io_conservation_report(self, param, lterminal) logical, intent(in) :: lterminal !! Indicates whether to output information to the terminal screen ! Internals real(DP), dimension(NDIM) :: Ltot_now, Lorbit_now, Lspin_now - real(DP), dimension(NDIM), save :: Ltot_last, Lorbit_last, Lspin_last - real(DP), save :: ke_orbit_last, ke_spin_last, pe_last, Eorbit_last real(DP) :: ke_orbit_now, ke_spin_now, pe_now, Eorbit_now real(DP) :: Eorbit_error, Etotal_error, Ecoll_error - real(DP) :: Mtot_now, Merror - real(DP) :: Lmag_now, Lerror + real(DP) :: GMtot_now + real(DP) :: Lerror, Merror + character(len=STRMAX) :: errmsg character(len=*), parameter :: EGYFMT = '(ES23.16,10(",",ES23.16,:))' ! Format code for all simulation output character(len=*), parameter :: EGYHEADER = '("t,Eorbit,Ecollisions,Lx,Ly,Lz,Mtot")' integer(I4B), parameter :: EGYIU = 72 @@ -27,68 +26,66 @@ module subroutine io_conservation_report(self, param, lterminal) "; D(Eorbit+Ecollisions)/|E0| = ", ES12.5, & "; DM/M0 = ", ES12.5)' - associate(system => self, pl => self%pl, cb => self%cb, npl => self%pl%nbody, Ecollisions => self%Ecollisions, Lescape => self%Lescape, Mescape => self%Mescape, & - Euntracked => self%Euntracked, Eorbit_orig => param%Eorbit_orig, Mtot_orig => param%Mtot_orig, & - Ltot_orig => param%Ltot_orig(:), Lmag_orig => param%Lmag_orig, Lorbit_orig => param%Lorbit_orig(:), Lspin_orig => param%Lspin_orig(:), & - lfirst => param%lfirstenergy) - if (param%energy_out /= "") then - if (lfirst .and. (param%out_stat /= "OLD")) then - open(unit = EGYIU, file = param%energy_out, form = "formatted", status = "replace", action = "write") + associate(system => self, pl => self%pl, cb => self%cb, npl => self%pl%nbody) + if ((param%out_type == REAL4_TYPE) .or. (param%out_type == REAL8_TYPE) .and. (param%energy_out /= "")) then + if (param%lfirstenergy .and. (param%out_stat /= "OLD")) then + open(unit = EGYIU, file = param%energy_out, form = "formatted", status = "replace", action = "write", err = 667, iomsg = errmsg) + write(EGYIU,EGYHEADER, err = 667, iomsg = errmsg) else - open(unit = EGYIU, file = param%energy_out, form = "formatted", status = "old", action = "write", position = "append") - write(EGYIU,EGYHEADER) + open(unit = EGYIU, file = param%energy_out, form = "formatted", status = "old", action = "write", position = "append", err = 667, iomsg = errmsg) end if end if - call pl%h2b(cb) + call pl%vb2vh(cb) + call pl%xh2xb(cb) call system%get_energy_and_momentum(param) ke_orbit_now = system%ke_orbit ke_spin_now = system%ke_spin pe_now = system%pe - Lorbit_now = system%Lorbit - Lspin_now = system%Lspin + Lorbit_now(:) = system%Lorbit(:) + Lspin_now(:) = system%Lspin(:) Eorbit_now = ke_orbit_now + ke_spin_now + pe_now - Ltot_now(:) = Lorbit_now(:) + Lspin_now(:) + Lescape(:) - Mtot_now = cb%mass + sum(pl%mass(1:npl)) + system%Mescape - if (lfirst) then - Eorbit_orig = Eorbit_now - Mtot_orig = Mtot_now - Lorbit_orig(:) = Lorbit_now(:) - Lspin_orig(:) = Lspin_now(:) - Ltot_orig(:) = Ltot_now(:) - Lmag_orig = norm2(Ltot_orig(:)) - lfirst = .false. + Ltot_now(:) = system%Ltot(:) + param%Lescape(:) + GMtot_now = system%GMtot + param%GMescape + + if (param%lfirstenergy) then + param%Eorbit_orig = Eorbit_now + param%GMtot_orig = GMtot_now + param%Lorbit_orig(:) = Lorbit_now(:) + param%Lspin_orig(:) = Lspin_now(:) + param%Ltot_orig(:) = Ltot_now(:) + param%lfirstenergy = .false. end if - if (param%energy_out /= "") then - write(EGYIU,EGYFMT) param%t, Eorbit_now, Ecollisions, Ltot_now, Mtot_now - close(EGYIU) + if ((param%out_type == REAL4_TYPE) .or. (param%out_type == REAL8_TYPE) .and. (param%energy_out /= "")) then + write(EGYIU,EGYFMT, err = 667, iomsg = errmsg) param%t, Eorbit_now, param%Ecollisions, Ltot_now, GMtot_now + close(EGYIU, err = 667, iomsg = errmsg) end if - if (.not.lfirst .and. lterminal) then - Lmag_now = norm2(Ltot_now) - Lerror = norm2(Ltot_now - Ltot_orig) / Lmag_orig - Eorbit_error = (Eorbit_now - Eorbit_orig) / abs(Eorbit_orig) - Ecoll_error = Ecollisions / abs(Eorbit_orig) - Etotal_error = (Eorbit_now - Ecollisions - Eorbit_orig - Euntracked) / abs(Eorbit_orig) - Merror = (Mtot_now - Mtot_orig) / Mtot_orig - write(*, egytermfmt) Lerror, Ecoll_error, Etotal_error, Merror - if (Ecoll_error > 0.0_DP) then - write(*,*) 'Something has gone wrong! Collisional energy should not be positive!' - write(*,*) 'dke_orbit: ',(ke_orbit_now - ke_orbit_last) / abs(Eorbit_orig) - write(*,*) 'dke_spin : ',(ke_spin_now - ke_spin_last) / abs(Eorbit_orig) - write(*,*) 'dpe : ',(pe_now - pe_last) / abs(Eorbit_orig) - write(*,*) + + if (.not.param%lfirstenergy) then + Lerror = norm2(Ltot_now(:) - param%Ltot_orig(:)) / norm2(param%Ltot_orig(:)) + Eorbit_error = (Eorbit_now - param%Eorbit_orig) / abs(param%Eorbit_orig) + Ecoll_error = param%Ecollisions / abs(param%Eorbit_orig) + Etotal_error = (Eorbit_now - param%Ecollisions - param%Eorbit_orig - param%Euntracked) / abs(param%Eorbit_orig) + Merror = (GMtot_now - param%GMtot_orig) / param%GMtot_orig + if (lterminal) write(*, EGYTERMFMT) Lerror, Ecoll_error, Etotal_error, Merror + if (abs(Merror) > 100 * epsilon(Merror)) then + write(*,*) "Severe error! Mass not conserved! Halting!" + call pl%xv2el(cb) + call param%nciu%open(param) + call self%write_hdr(param%nciu, param) + call cb%write_frame(param%nciu, param) + call pl%write_frame(param%nciu, param) + call param%nciu%close(param) + call util_exit(FAILURE) end if end if - ke_orbit_last = ke_orbit_now - ke_spin_last = ke_spin_now - pe_last = pe_now - Eorbit_last = Eorbit_now - Lorbit_last(:) = Lorbit_now(:) - Lspin_last(:) = Lspin_now(:) - Ltot_last(:) = Ltot_now(:) end associate + return + 667 continue + write(*,*) "Error writing energy and momentum tracking file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_conservation_report @@ -105,31 +102,120 @@ module subroutine io_dump_param(self, param_file_name) character(len=*), intent(in) :: param_file_name !! Parameter input file name (i.e. param.in) ! Internals integer(I4B), parameter :: LUN = 7 !! Unit number of output file - integer(I4B) :: ierr !! Error code - character(STRMAX) :: error_message !! Error message in UDIO procedure - - open(unit = LUN, file = param_file_name, status='replace', form = 'FORMATTED', iostat =ierr) - if (ierr /=0) then - write(*,*) 'Swiftest error.' - write(*,*) ' Could not open dump file: ',trim(adjustl(param_file_name)) - call util_exit(FAILURE) - end if - + character(STRMAX) :: errmsg !! Error message in UDIO procedure + integer(I4B) :: ierr + + open(unit = LUN, file = param_file_name, status='replace', form = 'FORMATTED', err = 667, iomsg = errmsg) !! todo: Currently this procedure does not work in user-defined derived-type input mode !! due to compiler incompatabilities !write(LUN,'(DT)') param - call self%writer(LUN, iotype = "none", v_list = [0], iostat = ierr, iomsg = error_message) - if (ierr /= 0) then - write(*,*) trim(adjustl(error_message)) - call util_exit(FAILURE) + call self%writer(LUN, iotype = "none", v_list = [0], iostat = ierr, iomsg = errmsg) + if (ierr == 0) then + close(LUN, err = 667, iomsg = errmsg) + return end if - close(LUN) - return + 667 continue + write(*,*) "Error opening parameter dump file " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_dump_param - module subroutine io_dump_swiftest(self, param) + module subroutine io_dump_particle_info(self, iu) + !! author: David A. Minton + !! + !! Reads in particle information object information from an open file unformatted file + implicit none + ! Arguments + class(swiftest_particle_info), intent(in) :: self !! Particle metadata information object + integer(I4B), intent(in) :: iu !! Open file unit number + ! Internals + character(STRMAX) :: errmsg + + write(iu, err = 667, iomsg = errmsg) self%name + write(iu, err = 667, iomsg = errmsg) self%particle_type + write(iu, err = 667, iomsg = errmsg) self%origin_type + write(iu, err = 667, iomsg = errmsg) self%origin_time + write(iu, err = 667, iomsg = errmsg) self%origin_xh(:) + write(iu, err = 667, iomsg = errmsg) self%origin_vh(:) + + return + + 667 continue + write(*,*) "Error writing particle metadata information from file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_dump_particle_info + + + module subroutine io_dump_particle_info_base(self, param, idx) + !! author: David A. Minton + !! + !! Dumps the particle information data to a file. + !! Pass a list of array indices for test particles (tpidx) and/or massive bodies (plidx) to append + implicit none + ! Arguments + class(swiftest_base), intent(inout) :: self !! Swiftest base object (can be cb, pl, or tp) + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + integer(I4B), dimension(:), optional, intent(in) :: idx !! Array of test particle indices to append to the particle file + + ! Internals + logical, save :: lfirst = .true. + integer(I4B), parameter :: LUN = 22 + integer(I4B) :: i + character(STRMAX) :: errmsg + + !if ((param%out_type == REAL4_TYPE) .or. (param%out_type == REAL8_TYPE)) then + if (lfirst) then + select case(param%out_stat) + case('APPEND') + open(unit = LUN, file = param%particle_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + case('NEW', 'UNKNOWN', 'REPLACE') + open(unit = LUN, file = param%particle_out, status = param%out_stat, form = 'UNFORMATTED', err = 667, iomsg = errmsg) + case default + write(*,*) 'Invalid status code',trim(adjustl(param%out_stat)) + call util_exit(FAILURE) + end select + + lfirst = .false. + else + open(unit = LUN, file = param%particle_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + end if + + select type(self) + class is (swiftest_cb) + write(LUN, err = 667, iomsg = errmsg) self%id + call self%info%dump(LUN) + class is (swiftest_body) + if (present(idx)) then + do i = 1, size(idx) + write(LUN, err = 667, iomsg = errmsg) self%id(idx(i)) + call self%info(idx(i))%dump(LUN) + end do + else + do i = 1, self%nbody + write(LUN, err = 667, iomsg = errmsg) self%id(i) + call self%info(i)%dump(LUN) + end do + end if + end select + + close(unit = LUN, err = 667, iomsg = errmsg) + !else if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + call param%nciu%open(param) + call self%write_particle_info(param%nciu) + call param%nciu%close(param) + end if + + return + + 667 continue + write(*,*) "Error reading central body file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_dump_particle_info_base + + + module subroutine io_dump_base(self, param) !! author: David A. Minton !! !! Dump massive body data to files @@ -145,6 +231,7 @@ module subroutine io_dump_swiftest(self, param) integer(I4B),parameter :: LUN = 7 !! Unit number for dump file integer(I4B) :: iu = LUN character(len=:), allocatable :: dump_file_name + character(STRMAX) :: errmsg select type(self) class is(swiftest_cb) @@ -154,17 +241,22 @@ module subroutine io_dump_swiftest(self, param) class is (swiftest_tp) dump_file_name = trim(adjustl(param%intpfile)) end select - open(unit = iu, file = dump_file_name, form = "UNFORMATTED", status = 'replace', iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " Unable to open binary dump file " // dump_file_name - call util_exit(FAILURE) - end if - call self%write_frame(iu, param) - close(LUN) + open(unit = iu, file = dump_file_name, form = "UNFORMATTED", status = 'replace', err = 667, iomsg = errmsg) + select type(self) + class is (swiftest_body) + write(iu, err = 667, iomsg = errmsg) self%nbody + call io_write_frame_body(self,iu, param) + class is (swiftest_cb) + call io_write_frame_cb(self,iu, param) + end select + close(iu, err = 667, iomsg = errmsg) return - end subroutine io_dump_swiftest + + 667 continue + write(*,*) "Error dumping body data to file " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_dump_base module subroutine io_dump_system(self, param) @@ -183,48 +275,45 @@ module subroutine io_dump_system(self, param) integer(I4B), save :: idx = 1 !! Index of current dump file. Output flips between 2 files for extra security !! in case the program halts during writing character(len=:), allocatable :: param_file_name - real(DP) :: deltawall, wallperstep, tfrac - integer(I8B) :: clock_count, count_rate, count_max + real(DP) :: tfrac character(*), parameter :: statusfmt = '("Time = ", ES12.5, "; fraction done = ", F6.3, "; Number of active pl, tp = ", I5, ", ", I5)' - character(len=*), parameter :: walltimefmt = '(" Wall time (s): ", es12.5, "; Wall time/step in this interval (s): ", es12.5)' + character(*), parameter :: symbastatfmt = '("Time = ", ES12.5, "; fraction done = ", F6.3, "; Number of active plm, pl, tp = ", I5, ", ", I5, ", ", I5)' logical, save :: lfirst = .true. - real(DP), save :: start, finish if (lfirst) then - call system_clock(clock_count, count_rate, count_max) - start = clock_count / (count_rate * 1.0_DP) - finish = start lfirst = .false. + if (param%lenergy) call self%conservation_report(param, lterminal=.false.) else allocate(dump_param, source=param) param_file_name = trim(adjustl(DUMP_PARAM_FILE(idx))) dump_param%incbfile = trim(adjustl(DUMP_CB_FILE(idx))) dump_param%inplfile = trim(adjustl(DUMP_PL_FILE(idx))) dump_param%intpfile = trim(adjustl(DUMP_TP_FILE(idx))) - dump_param%out_form = XV + dump_param%in_form = XV dump_param%out_stat = 'APPEND' + dump_param%in_type = REAL8_TYPE dump_param%T0 = param%t + call dump_param%dump(param_file_name) + dump_param%out_form = XV call self%cb%dump(dump_param) - if (self%pl%nbody > 0) call self%pl%dump(dump_param) - if (self%tp%nbody > 0) call self%tp%dump(dump_param) + call self%pl%dump(dump_param) + call self%tp%dump(dump_param) idx = idx + 1 if (idx > NDUMPFILES) idx = 1 tfrac = (param%t - param%t0) / (param%tstop - param%t0) - call system_clock(clock_count, count_rate, count_max) - deltawall = clock_count / (count_rate * 1.0_DP) - finish - wallperstep = deltawall / param%istep_dump - finish = clock_count / (count_rate * 1.0_DP) - write(*, statusfmt) param%t, tfrac, self%pl%nbody, self%tp%nbody - write(*, walltimefmt) finish - start, wallperstep - if (param%lenergy) call self%conservation_report(param, lterminal=.true.) + select type(pl => self%pl) + class is (symba_pl) + write(*, symbastatfmt) param%t, tfrac, pl%nplm, pl%nbody, self%tp%nbody + class default + write(*, statusfmt) param%t, tfrac, pl%nbody, self%tp%nbody + end select end if - return end subroutine io_dump_system @@ -292,6 +381,45 @@ module function io_get_args(integrator, param_file_name) result(ierr) end function io_get_args + module function io_get_old_t_final_system(self, param) result(old_t_final) + !! author: David A. Minton + !! + !! Validates the dump file to check whether the dump file initial conditions duplicate the last frame of the binary output. + !! + implicit none + ! Arguments + class(swiftest_nbody_system), intent(in) :: self + class(swiftest_parameters), intent(in) :: param + ! Result + real(DP) :: old_t_final + ! Internals + class(swiftest_nbody_system), allocatable :: tmpsys + class(swiftest_parameters), allocatable :: tmpparam + integer(I4B), parameter :: LUN = 76 + integer(I4B) :: ierr, iu = LUN + character(len=STRMAX) :: errmsg + + old_t_final = 0.0_DP + allocate(tmpsys, source=self) + allocate(tmpparam, source=param) + + ierr = 0 + open(unit = iu, file = param%outfile, status = 'OLD', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + do + ierr = tmpsys%read_frame(iu, tmpparam) + if (ierr /= 0) exit + end do + if (is_iostat_end(ierr)) then + old_t_final = tmpparam%t + return + end if + + 667 continue + write(*,*) "Error reading binary output file. " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end function io_get_old_t_final_system + + module function io_get_token(buffer, ifirst, ilast, ierr) result(token) !! author: David A. Minton !! @@ -368,11 +496,12 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) character(STRMAX) :: line !! Line of the input file character (len=:), allocatable :: line_trim,param_name, param_value !! Strings used to parse the param file character(*),parameter :: linefmt = '(A)' !! Format code for simple text string + ! Parse the file line by line, extracting tokens then matching them up with known parameters if possible associate(param => self) do - read(unit = unit, fmt = linefmt, iostat = iostat, end = 1) line + read(unit = unit, fmt = linefmt, end = 1, err = 667, iomsg = iomsg) line line_trim = trim(adjustl(line)) ilength = len(line_trim) if ((ilength /= 0)) then @@ -385,13 +514,13 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) param_value = io_get_token(line_trim, ifirst, ilast, iostat) select case (param_name) case ("T0") - read(param_value, *) param%t0 + read(param_value, *, err = 667, iomsg = iomsg) param%t0 t0_set = .true. case ("TSTOP") - read(param_value, *) param%tstop + read(param_value, *, err = 667, iomsg = iomsg) param%tstop tstop_set = .true. case ("DT") - read(param_value, *) param%dt + read(param_value, *, err = 667, iomsg = iomsg) param%dt dt_set = .true. case ("CB_IN") param%incbfile = param_value @@ -402,6 +531,9 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) case ("IN_TYPE") call io_toupper(param_value) param%in_type = param_value + case ("IN_FORM") + call io_toupper(param_value) + param%in_form = param_value case ("ISTEP_OUT") read(param_value, *) param%istep_out case ("BIN_OUT") @@ -416,26 +548,26 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) call io_toupper(param_value) param%out_stat = param_value case ("ISTEP_DUMP") - read(param_value, *) param%istep_dump + read(param_value, *, err = 667, iomsg = iomsg) param%istep_dump case ("CHK_CLOSE") call io_toupper(param_value) if (param_value == "YES" .or. param_value == 'T') param%lclose = .true. case ("CHK_RMIN") - read(param_value, *) param%rmin + read(param_value, *, err = 667, iomsg = iomsg) param%rmin case ("CHK_RMAX") - read(param_value, *) param%rmax + read(param_value, *, err = 667, iomsg = iomsg) param%rmax case ("CHK_EJECT") - read(param_value, *) param%rmaxu + read(param_value, *, err = 667, iomsg = iomsg) param%rmaxu case ("CHK_QMIN") - read(param_value, *) param%qmin + read(param_value, *, err = 667, iomsg = iomsg) param%qmin case ("CHK_QMIN_COORD") call io_toupper(param_value) param%qmin_coord = param_value case ("CHK_QMIN_RANGE") - read(param_value, *) param%qmin_alo + read(param_value, *, err = 667, iomsg = iomsg) param%qmin_alo ifirst = ilast + 1 param_value = io_get_token(line, ifirst, ilast, iostat) - read(param_value, *) param%qmin_ahi + read(param_value, *, err = 667, iomsg = iomsg) param%qmin_ahi case ("ENC_OUT") param%enc_out = param_value case ("DISCARD_OUT") @@ -452,11 +584,11 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) call io_toupper(param_value) if (param_value == "YES" .or. param_value == 'T' ) param%lrhill_present = .true. case ("MU2KG") - read(param_value, *) param%MU2KG + read(param_value, *, err = 667, iomsg = iomsg) param%MU2KG case ("TU2S") - read(param_value, *) param%TU2S + read(param_value, *, err = 667, iomsg = iomsg) param%TU2S case ("DU2M") - read(param_value, *) param%DU2M + read(param_value, *, err = 667, iomsg = iomsg) param%DU2M case ("ENERGY") call io_toupper(param_value) if (param_value == "YES" .or. param_value == 'T') param%lenergy = .true. @@ -476,47 +608,50 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) call io_toupper(param_value) if (param_value == "NO" .or. param_value == 'F') param%lfirstenergy = .false. case("EORBIT_ORIG") - read(param_value, *) param%Eorbit_orig - case("MTOT_ORIG") - read(param_value, *) param%Mtot_orig + read(param_value, *, err = 667, iomsg = iomsg) param%Eorbit_orig + case("GMTOT_ORIG") + read(param_value, *, err = 667, iomsg = iomsg) param%GMtot_orig case("LTOT_ORIG") - read(param_value, *) param%Ltot_orig(1) + read(param_value, *, err = 667, iomsg = iomsg) param%Ltot_orig(1) do i = 2, NDIM - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) - read(param_value, *) param%Ltot_orig(i) + read(param_value, *, err = 667, iomsg = iomsg) param%Ltot_orig(i) end do - param%Lmag_orig = norm2(param%Ltot_orig(:)) case("LORBIT_ORIG") - read(param_value, *) param%Lorbit_orig(1) + read(param_value, *, err = 667, iomsg = iomsg) param%Lorbit_orig(1) do i = 2, NDIM - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) - read(param_value, *) param%Lorbit_orig(i) + read(param_value, *, err = 667, iomsg = iomsg) param%Lorbit_orig(i) end do case("LSPIN_ORIG") - read(param_value, *) param%Lspin_orig(1) + read(param_value, *, err = 667, iomsg = iomsg) param%Lspin_orig(1) do i = 2, NDIM - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) - read(param_value, *) param%Lspin_orig(i) + read(param_value, *, err = 667, iomsg = iomsg) param%Lspin_orig(i) end do case("LESCAPE") - read(param_value, *) param%Lescape(1) + read(param_value, *, err = 667, iomsg = iomsg) param%Lescape(1) do i = 2, NDIM - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) - read(param_value, *) param%Lescape(i) + read(param_value, *, err = 667, iomsg = iomsg) param%Lescape(i) end do - case("MESCAPE") - read(param_value, *) param%Mescape + case("GMESCAPE") + read(param_value, *, err = 667, iomsg = iomsg) param%GMescape case("ECOLLISIONS") - read(param_value, *) param%Ecollisions + read(param_value, *, err = 667, iomsg = iomsg) param%Ecollisions case("EUNTRACKED") - read(param_value, *) param%Euntracked - case ("NPLMAX", "NTPMAX", "GMTINY", "PARTICLE_OUT", "FRAGMENTATION", "SEED", "YARKOVSKY", "YORP") ! Ignore SyMBA-specific, not-yet-implemented, or obsolete input parameters + read(param_value, *, err = 667, iomsg = iomsg) param%Euntracked + case ("MAXID") + read(param_value, *, err = 667, iomsg = iomsg) param%maxid + case ("PARTICLE_OUT") + param%particle_out = param_value + case ("NPLMAX", "NTPMAX", "GMTINY", "MIN_GMFRAG", "FRAGMENTATION", "SEED", "YARKOVSKY", "YORP") ! Ignore SyMBA-specific, not-yet-implemented, or obsolete input parameters case default - write(iomsg,*) "Unknown parameter -> ",param_name + write(*,*) "Unknown parameter -> ",param_name iostat = -1 return end select @@ -559,12 +694,12 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) param%lrestart = (param%out_stat == "APPEND") if (param%outfile /= "") then if ((param%out_type /= REAL4_TYPE) .and. (param%out_type /= REAL8_TYPE) .and. & - (param%out_type /= SWIFTER_REAL4_TYPE) .and. (param%out_type /= SWIFTER_REAL8_TYPE)) then + (param%out_type /= NETCDF_FLOAT_TYPE) .and. (param%out_type /= NETCDF_DOUBLE_TYPE)) then write(iomsg,*) 'Invalid out_type: ',trim(adjustl(param%out_type)) iostat = -1 return end if - if ((param%out_form /= "EL") .and. (param%out_form /= "XV")) then + if ((param%out_form /= "EL") .and. (param%out_form /= "XV") .and. (param%out_form /= "XVEL")) then write(iomsg,*) 'Invalid out_form: ',trim(adjustl(param%out_form)) iostat = -1 return @@ -574,7 +709,6 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) iostat = -1 return end if - end if if (param%qmin > 0.0_DP) then if ((param%qmin_coord /= "HELIO") .and. (param%qmin_coord /= "BARY")) then @@ -605,23 +739,32 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) write(*,*) "BIN_OUT = ",trim(adjustl(param%outfile)) write(*,*) "OUT_TYPE = ",trim(adjustl(param%out_type)) write(*,*) "OUT_FORM = ",trim(adjustl(param%out_form)) + write(*,*) "IN_FORM = ",trim(adjustl(param%in_form)) write(*,*) "OUT_STAT = ",trim(adjustl(param%out_stat)) write(*,*) "ISTEP_DUMP = ",param%istep_dump write(*,*) "CHK_CLOSE = ",param%lclose - write(*,*) "CHK_RMIN = ",param%rmin - write(*,*) "CHK_RMAX = ",param%rmax - write(*,*) "CHK_EJECT = ",param%rmaxu - write(*,*) "CHK_QMIN = ",param%qmin - write(*,*) "CHK_QMIN_COORD = ",trim(adjustl(param%qmin_coord)) - write(*,*) "CHK_QMIN_RANGE = ",param%qmin_alo, param%qmin_ahi + if (param%rmin > 0.0) then + write(*,*) "CHK_RMIN = ",param%rmin + else + write(*,*) "! CHK_RMIN value will be the central body radius" + end if + if (param%rmax > 0.0_DP) write(*,*) "CHK_RMAX = ",param%rmax + if (param%rmaxu > 0.0_DP) write(*,*) "CHK_EJECT = ",param%rmaxu + if ((param%qmin > 0.0_DP) .or. (param%qmin_alo > 0.0_DP) .or. (param%qmin_ahi > 0.0_DP)) write(*,*) "CHK_QMIN_COORD = ",trim(adjustl(param%qmin_coord)) + if (param%qmin > 0.0_DP) write(*,*) "CHK_QMIN = ",param%qmin + if ((param%qmin_alo > 0.0_DP) .or. (param%qmin_ahi > 0.0_DP)) write(*,*) "CHK_QMIN_RANGE = ",param%qmin_alo, param%qmin_ahi write(*,*) "EXTRA_FORCE = ",param%lextra_force write(*,*) "RHILL_PRESENT = ",param%lrhill_present write(*,*) "ROTATION = ", param%lrotation write(*,*) "TIDES = ", param%ltides write(*,*) "ENERGY = ",param%lenergy + if (param%lenergy) write(*,*) "ENERGY_OUT = ",trim(adjustl(param%energy_out)) write(*,*) "MU2KG = ",param%MU2KG write(*,*) "TU2S = ",param%TU2S write(*,*) "DU2M = ",param%DU2M + if (trim(adjustl(param%outfile)) == "") then + param%outfile = BIN_OUTFILE + end if if (trim(adjustl(param%enc_out)) /= "") then write(*,*) "ENC_OUT = ",trim(adjustl(param%enc_out)) else @@ -632,6 +775,7 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) write(*,*) "BIG_DISCARD = ",param%lbig_discard else write(*,*) "! DISCARD_OUT not set: Discards will not be recorded to file" + param%lbig_discard = .false. write(*,*) "! BIG_DISCARD = ",param%lbig_discard end if @@ -643,13 +787,14 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) ! Calculate the G for the system units param%GU = GC / (param%DU2M**3 / (param%MU2KG * param%TU2S**2)) - - ! Calculate the inverse speed of light in the system units - param%inv_c2 = einsteinC * param%TU2S / param%DU2M - param%inv_c2 = (param%inv_c2)**(-2) + if (param%lgr) then + ! Calculate the inverse speed of light in the system units + param%inv_c2 = einsteinC * param%TU2S / param%DU2M + param%inv_c2 = (param%inv_c2)**(-2) + end if associate(integrator => v_list(1)) - if (integrator == RMVS) then + if ((integrator == RMVS) .or. (integrator == SYMBA)) then if (.not.param%lclose) then write(iomsg,*) 'This integrator requires CHK_CLOSE to be enabled.' iostat = -1 @@ -670,6 +815,7 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) iostat = 0 end associate + 667 continue return end subroutine io_param_reader @@ -693,10 +839,9 @@ module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg) ! Internals character(*),parameter :: Ifmt = '(I0)' !! Format label for integer values character(*),parameter :: Rfmt = '(ES25.17)' !! Format label for real values - character(*),parameter :: Rarrfmt = '(3(ES25.17,1X))' !! Format label for real values character(*),parameter :: Lfmt = '(L1)' !! Format label for logical values - character(len=*), parameter :: Afmt = '(A25,1X,64(:,A25,1X))' - character(256) :: param_name, param_value + character(len=NAMELEN) :: param_name + character(LEN=STRMAX) :: param_value, v1, v2, v3 type character_array character(25) :: value end type character_array @@ -704,72 +849,88 @@ module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg) integer(I4B) :: i associate(param => self) - write(param_name, Afmt) "T0"; write(param_value,Rfmt) param%t0; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "TSTOP"; write(param_value, Rfmt) param%tstop; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "DT"; write(param_value, Rfmt) param%dt; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "PL_IN"; write(param_value, Afmt) trim(adjustl(param%inplfile)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "TP_in"; write(param_value, Afmt) trim(adjustl(param%intpfile)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "IN_TYPE"; write(param_value, Afmt) trim(adjustl(param%in_type)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "T0"; write(param_value,Rfmt) param%t0; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "TSTOP"; write(param_value, Rfmt) param%tstop; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "DT"; write(param_value, Rfmt) param%dt; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "CB_IN"; write(param_value, *) trim(adjustl(param%incbfile)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "PL_IN"; write(param_value, *) trim(adjustl(param%inplfile)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "TP_IN"; write(param_value, *) trim(adjustl(param%intpfile)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "IN_TYPE"; write(param_value, *) trim(adjustl(param%in_type)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "IN_FORM"; write(param_value, *) trim(adjustl(param%in_form)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + if (param%istep_dump > 0) write(param_name, *) "ISTEP_DUMP"; write(param_value, Ifmt) param%istep_dump; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) if (param%istep_out > 0) then - write(param_name, Afmt) "ISTEP_OUT"; write(param_value, Ifmt) param%istep_out; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "BIN_OUT"; write(param_value, Afmt) trim(adjustl(param%outfile)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "OUT_TYPE"; write(param_value, Afmt) trim(adjustl(param%out_type)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "OUT_FORM"; write(param_value, Afmt) trim(adjustl(param%out_form)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "OUT_STAT"; write(param_value, Afmt) "APPEND"; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "ISTEP_OUT"; write(param_value, Ifmt) param%istep_out; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "BIN_OUT"; write(param_value, *) trim(adjustl(param%outfile)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "OUT_TYPE"; write(param_value, *) trim(adjustl(param%out_type)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "OUT_FORM"; write(param_value, *) trim(adjustl(param%out_form)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "OUT_STAT"; write(param_value, *) "APPEND"; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) end if - write(param_name, Afmt) "ENC_OUT"; write(param_value, Afmt) trim(adjustl(param%enc_out)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - if (param%istep_dump > 0) then - write(param_name, Afmt) "ISTEP_DUMP"; write(param_value, Ifmt) param%istep_dump; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "PARTICLE_OUT"; write(param_value, *) trim(adjustl(param%particle_out)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + if (param%enc_out /= "") then + write(param_name, *) "ENC_OUT"; write(param_value, *) trim(adjustl(param%enc_out)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) end if - write(param_name, Afmt) "CHK_RMIN"; write(param_value, Rfmt) param%rmin; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "CHK_RMAX"; write(param_value, Rfmt) param%rmax; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "CHK_EJECT"; write(param_value, Rfmt) param%rmaxu; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "CHK_QMIN"; write(param_value, Rfmt) param%qmin; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "CHK_RMIN"; write(param_value, Rfmt) param%rmin; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "CHK_RMAX"; write(param_value, Rfmt) param%rmax; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "CHK_EJECT"; write(param_value, Rfmt) param%rmaxu; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "CHK_QMIN"; write(param_value, Rfmt) param%qmin; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) if (param%qmin >= 0.0_DP) then - write(param_name, Afmt) "CHK_QMIN_COORD"; write(param_value, Afmt) trim(adjustl(param%qmin_coord)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "CHK_QMIN_COORD"; write(param_value, *) trim(adjustl(param%qmin_coord)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) allocate(param_array(2)) write(param_array(1)%value, Rfmt) param%qmin_alo write(param_array(2)%value, Rfmt) param%qmin_ahi - write(param_name, Afmt) "CHK_QMIN_RANGE"; write(unit, Afmt) adjustl(param_name), adjustl(param_array(1)%value), adjustl(param_array(2)%value) + write(param_name, *) "CHK_QMIN_RANGE"; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name), adjustl(param_array(1)%value), adjustl(param_array(2)%value) + end if + write(param_name, *) "MU2KG"; write(param_value, Rfmt) param%MU2KG; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "TU2S"; write(param_value, Rfmt) param%TU2S ; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "DU2M"; write(param_value, Rfmt) param%DU2M; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "RHILL_PRESENT"; write(param_value, Lfmt) param%lrhill_present; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "EXTRA_FORCE"; write(param_value, Lfmt) param%lextra_force; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + if (param%discard_out /= "") then + write(param_name, *) "DISCARD_OUT"; write(param_value, *) trim(adjustl(param%discard_out)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + end if + if (param%discard_out /= "") then + write(param_name, *) "BIG_DISCARD"; write(param_value, Lfmt) param%lbig_discard; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) end if - write(param_name, Afmt) "MU2KG"; write(param_value, Rfmt) param%MU2KG; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "TU2S"; write(param_value, Rfmt) param%TU2S ; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "DU2M"; write(param_value, Rfmt) param%DU2M; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "RHILL_PRESENT"; write(param_value, Lfmt) param%lrhill_present; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "EXTRA_FORCE"; write(param_value, Lfmt) param%lextra_force; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "BIG_DISCARD"; write(param_value, Lfmt) param%lbig_discard; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "CHK_CLOSE"; write(param_value, Lfmt) param%lclose; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "ENERGY"; write(param_value, Lfmt) param%lenergy; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "GR"; write(param_value, Lfmt) param%lgr; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "ROTATION"; write(param_value, Lfmt) param%lrotation; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "TIDES"; write(param_value, Lfmt) param%ltides; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "CHK_CLOSE"; write(param_value, Lfmt) param%lclose; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "ENERGY"; write(param_value, Lfmt) param%lenergy; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + if (param%lenergy .and. (param%energy_out /= "")) then + write(param_name, *) "ENERGY_OUT"; write(param_value, *) trim(adjustl(param%energy_out)); write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + end if + write(param_name, *) "GR"; write(param_value, Lfmt) param%lgr; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "ROTATION"; write(param_value, Lfmt) param%lrotation; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "TIDES"; write(param_value, Lfmt) param%ltides; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) if (param%lenergy) then - write(param_name, Afmt) "FIRSTENERGY"; write(param_value, Lfmt) param%lfirstenergy; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "EORBIT_ORIG"; write(param_value, Rfmt) param%Eorbit_orig; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "MTOT_ORIG"; write(param_value, Rfmt) param%Mtot_orig; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(unit, '("LTOT_ORIG ",3(1X,ES25.17))') param%Ltot_orig(:) - write(unit, '("LORBIT_ORIG",3(1X,ES25.17))') param%Lorbit_orig(:) - write(unit, '("LSPIN_ORIG ",3(1X,ES25.17))') param%Lspin_orig(:) - write(unit, '("LESCAPE ",3(1X,ES25.17))') param%Lescape(:) + write(param_name, *) "FIRSTENERGY"; write(param_value, Lfmt) param%lfirstenergy; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "EORBIT_ORIG"; write(param_value, Rfmt) param%Eorbit_orig; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "GMTOT_ORIG"; write(param_value, Rfmt) param%GMtot_orig; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "LTOT_ORIG"; write(v1, Rfmt) param%Ltot_orig(1); write(v2, Rfmt) param%Ltot_orig(2); write(v3, Rfmt) param%Ltot_orig(3) + write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(v1)) // " " // trim(adjustl(v2)) // " " // trim(adjustl(v3)) + write(param_name, *) "LORBIT_ORIG"; write(v1, Rfmt) param%Lorbit_orig(1); write(v2, Rfmt) param%Lorbit_orig(2); write(v3, Rfmt) param%Lorbit_orig(3) + write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(v1)) // " " // trim(adjustl(v2)) // " " // trim(adjustl(v3)) + write(param_name, *) "LSPIN_ORIG"; write(v1, Rfmt) param%Lspin_orig(1); write(v2, Rfmt) param%Lspin_orig(2); write(v3, Rfmt) param%Lspin_orig(3) + write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(v1)) // " " // trim(adjustl(v2)) // " " // trim(adjustl(v3)) + write(param_name, *) "LESCAPE"; write(v1, Rfmt) param%Lescape(1); write(v2, Rfmt) param%Lescape(2); write(v3, Rfmt) param%Lescape(3) + write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(v1)) // " " // trim(adjustl(v2)) // " " // trim(adjustl(v3)) - write(param_name, Afmt) "MESCAPE"; write(param_value, Rfmt) param%Mescape; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "ECOLLISIONS"; write(param_value, Rfmt) param%Ecollisions; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "EUNTRACKED"; write(param_value, Rfmt) param%Euntracked; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "GMESCAPE"; write(param_value, Rfmt) param%GMescape; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "ECOLLISIONS"; write(param_value, Rfmt) param%Ecollisions; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "EUNTRACKED"; write(param_value, Rfmt) param%Euntracked; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) end if - write(param_name, Afmt) "FIRSTKICK"; write(param_value, Lfmt) param%lfirstkick; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "FIRSTKICK"; write(param_value, Lfmt) param%lfirstkick; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "MAXID"; write(param_value, Ifmt) param%maxid; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) - - iostat = 0 iomsg = "UDIO not implemented" end associate + 667 continue + return end subroutine io_param_writer - module subroutine io_read_body_in(self, param) + module subroutine io_read_in_body(self, param) !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! !! Read in either test particle or massive body data @@ -783,11 +944,12 @@ module subroutine io_read_body_in(self, param) ! Internals integer(I4B), parameter :: LUN = 7 !! Unit number of input file integer(I4B) :: iu = LUN - integer(I4B) :: i, ierr, nbody + integer(I4B) :: i, nbody logical :: is_ascii, is_pl character(len=:), allocatable :: infile real(DP) :: t - real(QP) :: val + character(STRMAX) :: errmsg + integer(I4B) :: ierr ! Select the appropriate polymorphic class (test particle or massive body) select type(self) @@ -799,70 +961,41 @@ module subroutine io_read_body_in(self, param) is_pl = .false. end select - ierr = 0 is_ascii = (param%in_type == 'ASCII') select case(param%in_type) case(ASCII_TYPE) - open(unit = iu, file = infile, status = 'old', form = 'FORMATTED', iostat = ierr) - read(iu, *, iostat = ierr) nbody - call self%setup(nbody, param) - if (nbody > 0) then - do i = 1, nbody - select type(self) - class is (swiftest_pl) - if (param%lrhill_present) then - read(iu, *, iostat=ierr, err=100) self%id(i), val, self%rhill(i) - else - read(iu, *, iostat=ierr, err=100) self%id(i), val - end if - self%Gmass(i) = real(val, kind=DP) - self%mass(i) = real(val / param%GU, kind=DP) - if (param%lclose) read(iu, *, iostat=ierr, err=100) self%radius(i) - class is (swiftest_tp) - read(iu, *, iostat=ierr, err=100) self%id(i) - end select - read(iu, *, iostat=ierr, err=100) self%xh(1, i), self%xh(2, i), self%xh(3, i) - read(iu, *, iostat=ierr, err=100) self%vh(1, i), self%vh(2, i), self%vh(3, i) - select type (self) - class is (swiftest_pl) - if (param%lrotation) then - read(iu, *, iostat=ierr, err=100) self%Ip(1, i), self%Ip(2, i), self%Ip(3, i) - read(iu, *, iostat=ierr, err=100) self%rot(1, i), self%rot(2, i), self%rot(3, i) - end if - if (param%ltides) then - read(iu, *, iostat=ierr, err=100) self%k2(i) - read(iu, *, iostat=ierr, err=100) self%Q(i) - end if - end select - self%status(i) = ACTIVE - self%lmask(i) = .true. - end do - end if - case (REAL4_TYPE, REAL8_TYPE) !, SWIFTER_REAL4_TYPE, SWIFTER_REAL8_TYPE) - open(unit=iu, file=infile, status='old', form='UNFORMATTED', iostat=ierr) - read(iu, iostat=ierr, err=100) nbody - call self%setup(nbody, param) - if (nbody > 0) then - call self%read_frame(iu, param, XV, ierr) - self%status(:) = ACTIVE - self%lmask(:) = .true. - end if + open(unit = iu, file = infile, status = 'old', form = 'FORMATTED', err = 667, iomsg = errmsg) + read(iu, *, err = 667, iomsg = errmsg) nbody + case (REAL4_TYPE, REAL8_TYPE) + open(unit=iu, file=infile, status='old', form='UNFORMATTED', err = 667, iomsg = errmsg) + read(iu, err = 667, iomsg = errmsg) nbody case default - write(*,*) trim(adjustl(param%in_type)) // ' is an unrecognized file type' - ierr = -1 + write(errmsg,*) trim(adjustl(param%in_type)) // ' is an unrecognized file type' + goto 667 end select - close(iu) - 100 if (ierr /= 0 ) then - write(*,*) 'Error reading in initial conditions from ',trim(adjustl(infile)) - call util_exit(FAILURE) + call self%setup(nbody, param) + ierr = 0 + if (nbody > 0) then + ierr = self%read_frame(iu, param) + self%status(:) = ACTIVE + self%lmask(:) = .true. + do i = 1, nbody + call self%info(i)%set_value(status="ACTIVE") + end do end if + close(iu, err = 667, iomsg = errmsg) + + + if (ierr == 0) return + 667 continue + write(*,*) 'Error reading in initial conditions file: ',trim(adjustl(errmsg)) return - end subroutine io_read_body_in + end subroutine io_read_in_body - module subroutine io_read_cb_in(self, param) + module subroutine io_read_in_cb(self, param) !! author: David A. Minton !! !! Reads in central body data @@ -876,42 +1009,55 @@ module subroutine io_read_cb_in(self, param) ! Internals integer(I4B), parameter :: LUN = 7 !! Unit number of input file integer(I4B) :: iu = LUN - integer(I4B) :: ierr - logical :: is_ascii - real(DP) :: t - real(QP) :: val - - ierr = 0 - is_ascii = (param%in_type == 'ASCII') - if (is_ascii) then - open(unit = iu, file = param%incbfile, status = 'old', form = 'FORMATTED', iostat = ierr) - read(iu, *, iostat = ierr) self%id - read(iu, *, iostat = ierr) val - self%Gmass = real(val, kind=DP) - self%mass = real(val / param%GU, kind=DP) - read(iu, *, iostat = ierr) self%radius - read(iu, *, iostat = ierr) self%j2rp2 - read(iu, *, iostat = ierr) self%j4rp4 + character(len=STRMAX) :: errmsg + integer(I4B) :: ierr, idold + character(len=NAMELEN) :: name + + if (param%in_type == 'ASCII') then + self%id = 0 + param%maxid = 0 + open(unit = iu, file = param%incbfile, status = 'old', form = 'FORMATTED', err = 667, iomsg = errmsg) + read(iu, *, err = 667, iomsg = errmsg) name + call self%info%set_value(name=name) + read(iu, *, err = 667, iomsg = errmsg) self%Gmass + self%mass = real(self%Gmass / param%GU, kind=DP) + read(iu, *, err = 667, iomsg = errmsg) self%radius + read(iu, *, err = 667, iomsg = errmsg) self%j2rp2 + read(iu, *, err = 667, iomsg = errmsg) self%j4rp4 if (param%lrotation) then - read(iu, *, iostat = ierr) self%Ip(1), self%Ip(2), self%Ip(3) - read(iu, *, iostat = ierr) self%rot(1), self%rot(2), self%rot(3) + read(iu, *, err = 667, iomsg = errmsg) self%Ip(1), self%Ip(2), self%Ip(3) + read(iu, *, err = 667, iomsg = errmsg) self%rot(1), self%rot(2), self%rot(3) end if + ierr = 0 else - open(unit = iu, file = param%incbfile, status = 'old', form = 'UNFORMATTED', iostat = ierr) - call self%read_frame(iu, param, XV, ierr) - end if - close(iu) - if (ierr /= 0) then - write(*,*) 'Error opening massive body initial conditions file ',trim(adjustl(param%incbfile)) - call util_exit(FAILURE) + open(unit = iu, file = param%incbfile, status = 'old', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + ierr = self%read_frame(iu, param) end if - if (self%j2rp2 /= 0.0_DP) param%loblatecb = .true. + close(iu, err = 667, iomsg = errmsg) + + if (ierr == 0) then + + if (self%j2rp2 /= 0.0_DP) param%loblatecb = .true. + if (param%rmin < 0.0) param%rmin = self%radius + + select type(cb => self) + class is (symba_cb) + cb%GM0 = cb%Gmass + cb%dGM = 0.0_DP + cb%R0 = cb%radius + cb%L0(:) = cb%Ip(3) * cb%mass * cb%radius**2 * cb%rot(:) + end select + end if return - end subroutine io_read_cb_in + + 667 continue + write(*,*) "Error reading central body file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_read_in_cb - function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & + function io_read_encounter(t, id1, id2, Gmass1, Gmass2, radius1, radius2, & xh1, xh2, vh1, vh2, enc_out, out_type) result(ierr) !! author: David A. Minton !! @@ -921,8 +1067,8 @@ function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & !! Adapted from David E. Kaufmann's Swifter routine: io_read_encounter.f90 implicit none ! Arguments - integer(I4B), intent(out) :: name1, name2 - real(DP), intent(out) :: t, mass1, mass2, radius1, radius2 + integer(I4B), intent(out) :: id1, id2 + real(DP), intent(out) :: t, Gmass1, Gmass2, radius1, radius2 real(DP), dimension(:), intent(out) :: xh1, xh2, vh1, vh2 character(*), intent(in) :: enc_out, out_type ! Result @@ -947,12 +1093,12 @@ function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & return end if - read(iu, iostat = ierr) name1, xh1(1), xh1(2), xh1(3), vh1(1), vh1(2), vh1(3), mass1, radius1 + read(iu, iostat = ierr) id1, xh1(1), xh1(2), xh1(3), vh1(1), vh1(2), vh1(3), Gmass1, radius1 if (ierr /= 0) then close(unit = iu, iostat = ierr) return end if - read(iu, iostat = ierr) name2, xh2(2), xh2(2), xh2(3), vh2(2), vh2(2), vh2(3), mass2, radius2 + read(iu, iostat = ierr) id2, xh2(2), xh2(2), xh2(3), vh2(2), vh2(2), vh2(3), Gmass2, radius2 if (ierr /= 0) then close(unit = iu, iostat = ierr) return @@ -962,7 +1108,7 @@ function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & end function io_read_encounter - module subroutine io_read_frame_body(self, iu, param, form, ierr) + module function io_read_frame_body(self, iu, param) result(ierr) !! author: David A. Minton !! !! Reads a frame of output of either test particle or massive body data from a binary output file @@ -974,65 +1120,146 @@ module subroutine io_read_frame_body(self, iu, param, form, ierr) class(swiftest_body), intent(inout) :: self !! Swiftest particle object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code + ! Result + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + ! Internals + character(len=STRMAX) :: errmsg + character(len=NAMELEN), dimension(self%nbody) :: name + integer(I4B) :: i + real(QP) :: val + + if (self%nbody == 0) return + + if ((param%in_form /= EL) .and. (param%in_form /= XV)) then + write(errmsg, *) trim(adjustl(param%in_form)) // " is not a recognized format code for input files." + goto 667 + end if associate(n => self%nbody) - read(iu, iostat=ierr, err=100) self%id(:) - !read(iu, iostat=ierr, err=100) self%name(1:n) - select case (form) - case (EL) + + if (param%in_form == EL) then if (.not.allocated(self%a)) allocate(self%a(n)) if (.not.allocated(self%e)) allocate(self%e(n)) if (.not.allocated(self%inc)) allocate(self%inc(n)) if (.not.allocated(self%capom)) allocate(self%capom(n)) if (.not.allocated(self%omega)) allocate(self%omega(n)) if (.not.allocated(self%capm)) allocate(self%capm(n)) - read(iu, iostat=ierr, err=100) self%a(:) - read(iu, iostat=ierr, err=100) self%e(:) - read(iu, iostat=ierr, err=100) self%inc(:) - read(iu, iostat=ierr, err=100) self%capom(:) - read(iu, iostat=ierr, err=100) self%omega(:) - read(iu, iostat=ierr, err=100) self%capm(:) - case (XV) - read(iu, iostat=ierr, err=100) self%xh(1, :) - read(iu, iostat=ierr, err=100) self%xh(2, :) - read(iu, iostat=ierr, err=100) self%xh(3, :) - read(iu, iostat=ierr, err=100) self%vh(1, :) - read(iu, iostat=ierr, err=100) self%vh(2, :) - read(iu, iostat=ierr, err=100) self%vh(3, :) - end select - select type(pl => self) - class is (swiftest_pl) ! Additional output if the passed polymorphic object is a massive body - read(iu, iostat=ierr, err=100) pl%Gmass(:) - pl%mass(:) = pl%Gmass(:) / param%GU - if (param%lrhill_present) read(iu, iostat=ierr, err=100) pl%rhill(:) - if (param%lclose) read(iu, iostat=ierr, err=100) pl%radius(:) - if (param%lrotation) then - read(iu, iostat=ierr, err=100) pl%rot(1, :) - read(iu, iostat=ierr, err=100) pl%rot(2, :) - read(iu, iostat=ierr, err=100) pl%rot(3, :) - read(iu, iostat=ierr, err=100) pl%Ip(1, :) - read(iu, iostat=ierr, err=100) pl%Ip(2, :) - read(iu, iostat=ierr, err=100) pl%Ip(3, :) - end if - if (param%ltides) then - read(iu, iostat=ierr, err=100) pl%k2(1:n) - read(iu, iostat=ierr, err=100) pl%Q(1:n) - end if + end if + + select case(param%in_type) + case (REAL4_TYPE, REAL8_TYPE) + read(iu, err = 667, iomsg = errmsg) self%id(:) + read(iu, err = 667, iomsg = errmsg) name(:) + do i = 1, n + call self%info(i)%set_value(name=name(i)) + end do + + select case (param%in_form) + case (XV) + read(iu, err = 667, iomsg = errmsg) self%xh(1, :) + read(iu, err = 667, iomsg = errmsg) self%xh(2, :) + read(iu, err = 667, iomsg = errmsg) self%xh(3, :) + read(iu, err = 667, iomsg = errmsg) self%vh(1, :) + read(iu, err = 667, iomsg = errmsg) self%vh(2, :) + read(iu, err = 667, iomsg = errmsg) self%vh(3, :) + case (EL) + read(iu, err = 667, iomsg = errmsg) self%a(:) + read(iu, err = 667, iomsg = errmsg) self%e(:) + read(iu, err = 667, iomsg = errmsg) self%inc(:) + read(iu, err = 667, iomsg = errmsg) self%capom(:) + read(iu, err = 667, iomsg = errmsg) self%omega(:) + read(iu, err = 667, iomsg = errmsg) self%capm(:) + end select + + select type(pl => self) + class is (swiftest_pl) ! Additional output if the passed polymorphic object is a massive body + read(iu, err = 667, iomsg = errmsg) pl%Gmass(:) + pl%mass(:) = pl%Gmass(:) / param%GU + if (param%lrhill_present) read(iu, err = 667, iomsg = errmsg) pl%rhill(:) + read(iu, err = 667, iomsg = errmsg) pl%radius(:) + if (param%lrotation) then + read(iu, err = 667, iomsg = errmsg) pl%Ip(1, :) + read(iu, err = 667, iomsg = errmsg) pl%Ip(2, :) + read(iu, err = 667, iomsg = errmsg) pl%Ip(3, :) + read(iu, err = 667, iomsg = errmsg) pl%rot(1, :) + read(iu, err = 667, iomsg = errmsg) pl%rot(2, :) + read(iu, err = 667, iomsg = errmsg) pl%rot(3, :) + end if + if (param%ltides) then + read(iu, err = 667, iomsg = errmsg) pl%k2(:) + read(iu, err = 667, iomsg = errmsg) pl%Q(:) + end if + end select + + param%maxid = max(param%maxid, maxval(self%id(1:n))) + + case (ASCII_TYPE) + do i = 1, n + select type(self) + class is (swiftest_pl) + if (param%lrhill_present) then + read(iu, *, err = 667, iomsg = errmsg) name(i), val, self%rhill(i) + else + read(iu, *, err = 667, iomsg = errmsg) name(i), val + end if + call self%info(i)%set_value(name=name(i)) + self%Gmass(i) = real(val, kind=DP) + self%mass(i) = real(val / param%GU, kind=DP) + read(iu, *, err = 667, iomsg = errmsg) self%radius(i) + class is (swiftest_tp) + read(iu, *, err = 667, iomsg = errmsg) self%id(i) + end select + + select case(param%in_form) + case (XV) + read(iu, *, err = 667, iomsg = errmsg) self%xh(1, i), self%xh(2, i), self%xh(3, i) + read(iu, *, err = 667, iomsg = errmsg) self%vh(1, i), self%vh(2, i), self%vh(3, i) + case (EL) + read(iu, *, err = 667, iomsg = errmsg) self%a(i), self%e(i), self%inc(i) + read(iu, *, err = 667, iomsg = errmsg) self%capom(i), self%omega(i), self%capm(i) + end select + + select type (self) + class is (swiftest_pl) + if (param%lrotation) then + read(iu, *, err = 667, iomsg = errmsg) self%Ip(1, i), self%Ip(2, i), self%Ip(3, i) + read(iu, *, err = 667, iomsg = errmsg) self%rot(1, i), self%rot(2, i), self%rot(3, i) + end if + if (param%ltides) then + read(iu, *, err = 667, iomsg = errmsg) self%k2(i) + read(iu, *, err = 667, iomsg = errmsg) self%Q(i) + end if + end select + param%maxid = param%maxid + 1 + self%id(i) = param%maxid + end do end select - end associate - 100 if (ierr /=0) then - write(*,*) 'Error reading Swiftest body data' - call util_exit(FAILURE) - end if + if (param%in_form == EL) then + self%inc(1:n) = self%inc(1:n) * DEG2RAD + self%capom(1:n) = self%capom(1:n) * DEG2RAD + self%omega(1:n) = self%omega(1:n) * DEG2RAD + self%capm(1:n) = self%capm(1:n) * DEG2RAD + end if + end associate + ierr = 0 return - end subroutine io_read_frame_body + + 667 continue + select type (self) + class is (swiftest_pl) + write(*,*) "Error reading massive body file: " // trim(adjustl(errmsg)) + class is (swiftest_tp) + write(*,*) "Error reading test particle file: " // trim(adjustl(errmsg)) + class default + write(*,*) "Error reading body file: " // trim(adjustl(errmsg)) + end select + call util_exit(FAILURE) + end function io_read_frame_body - module subroutine io_read_frame_cb(self, iu, param, form, ierr) + module function io_read_frame_cb(self, iu, param) result(ierr) !! author: David A. Minton !! !! Reads a frame of output of central body data to the binary output file @@ -1044,71 +1271,87 @@ module subroutine io_read_frame_cb(self, iu, param, form, ierr) class(swiftest_cb), intent(inout) :: self !! Swiftest central body object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error cod + ! Result + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + ! Internals + character(len=STRMAX) :: errmsg + character(len=NAMELEN) :: name - read(iu, iostat=ierr, err=100) self%id - !read(iu, iostat=ierr, err=100) self%name - read(iu, iostat=ierr, err=100) self%Gmass + read(iu, err = 667, iomsg = errmsg) self%id + read(iu, err = 667, iomsg = errmsg) name + call self%info%set_value(name=name) + read(iu, err = 667, iomsg = errmsg) self%Gmass self%mass = self%Gmass / param%GU - read(iu, iostat=ierr, err=100) self%radius - read(iu, iostat=ierr, err=100) self%j2rp2 - read(iu, iostat=ierr, err=100) self%j4rp4 + read(iu, err = 667, iomsg = errmsg) self%radius + read(iu, err = 667, iomsg = errmsg) self%j2rp2 + read(iu, err = 667, iomsg = errmsg) self%j4rp4 if (param%lrotation) then - read(iu, iostat=ierr, err=100) self%Ip(:) - read(iu, iostat=ierr, err=100) self%rot(:) + read(iu, err = 667, iomsg = errmsg) self%Ip(1) + read(iu, err = 667, iomsg = errmsg) self%Ip(2) + read(iu, err = 667, iomsg = errmsg) self%Ip(3) + read(iu, err = 667, iomsg = errmsg) self%rot(1) + read(iu, err = 667, iomsg = errmsg) self%rot(2) + read(iu, err = 667, iomsg = errmsg) self%rot(3) end if if (param%ltides) then - read(iu, iostat=ierr, err=100) self%k2 - read(iu, iostat=ierr, err=100) self%Q - end if - 100 if (ierr /=0) then - write(*,*) 'Error reading central body data' - call util_exit(FAILURE) + read(iu, err = 667, iomsg = errmsg) self%k2 + read(iu, err = 667, iomsg = errmsg) self%Q end if + ierr = 0 return - end subroutine io_read_frame_cb + + 667 continue + write(*,*) "Error reading central body file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end function io_read_frame_cb - module subroutine io_read_frame_system(self, iu, param, form, ierr) + module function io_read_frame_system(self, iu, param) result(ierr) !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! !! Read a frame (header plus records for each massive body and active test particle) from a output binary file implicit none ! Arguments - class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object + integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code + ! Result + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful ! Internals - logical, save :: lfirst = .true. + character(len=STRMAX) :: errmsg + integer(I4B) :: npl, ntp - iu = BINUNIT - if (lfirst) then - open(unit = iu, file = param%outfile, status = 'OLD', form = 'UNFORMATTED', iostat = ierr) - lfirst = .false. - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " Binary output file already exists or cannot be accessed" - return - end if + ierr = io_read_hdr(iu, param%t, npl, ntp, param%out_form, param%out_type) + if (is_iostat_end(ierr)) return ! Reached the end of the frames + call self%pl%setup(npl, param) + call self%tp%setup(ntp, param) + + if (ierr /= 0) then + write(errmsg, *) "Cannot read frame header." + goto 667 end if - ierr = io_read_hdr(iu, param%t, self%pl%nbody, self%tp%nbody, param%out_form, param%out_type) + ierr = self%cb%read_frame(iu, param) if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " Binary output file already exists or cannot be accessed" - return + write(errmsg, *) "Cannot read central body frame." + goto 667 + end if + ierr = self%pl%read_frame(iu, param) + if (ierr /= 0) then + write(errmsg, *) "Cannot read massive body frame." + goto 667 + end if + ierr = self%tp%read_frame(iu, param) + if (ierr /= 0) then + write(errmsg, *) "Cannot read test particle frame." + goto 667 end if - call self%cb%read_frame(iu, param, form, ierr) - if (ierr /= 0) return - call self%pl%read_frame(iu, param, form, ierr) - if (ierr /= 0) return - call self%tp%read_frame(iu, param, form, ierr) return - end subroutine io_read_frame_system + + 667 continue + write(*,*) "Error reading system frame: " // trim(adjustl(errmsg)) + end function io_read_frame_system function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr) @@ -1122,33 +1365,41 @@ function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr) ! Arguments integer(I4B), intent(in) :: iu integer(I4B), intent(out) :: npl, ntp - character(*), intent(out) :: out_form + character(*), intent(out) :: out_form real(DP), intent(out) :: t character(*), intent(in) :: out_type ! Result integer(I4B) :: ierr ! Internals - real(SP) :: ttmp + real(SP) :: ttmp + character(len=STRMAX) :: errmsg select case (out_type) - case (REAL4_TYPE, SWIFTER_REAL4_TYPE) - read(iu, iostat = ierr) ttmp, npl, ntp, out_form - if (ierr /= 0) return + case (REAL4_TYPE) + read(iu, iostat = ierr, err = 667, iomsg = errmsg, end = 333) ttmp t = ttmp - case (REAL8_TYPE, SWIFTER_REAL8_TYPE) - read(iu, iostat = ierr) t - read(iu, iostat = ierr) npl - read(iu, iostat = ierr) ntp - read(iu, iostat = ierr) out_form + case (REAL8_TYPE) + read(iu, iostat = ierr, err = 667, iomsg = errmsg, end = 333) t case default - write(*,*) trim(adjustl(out_type)) // ' is an unrecognized file type' + write(errmsg,*) trim(adjustl(out_type)) // ' is an unrecognized file type' ierr = -1 end select + read(iu, iostat = ierr, err = 667, iomsg = errmsg) npl + read(iu, iostat = ierr, err = 667, iomsg = errmsg) ntp + read(iu, iostat = ierr, err = 667, iomsg = errmsg) out_form + + return + + 667 continue + write(*,*) "Error reading header: " // trim(adjustl(errmsg)) + 333 continue + return return end function io_read_hdr - module subroutine io_read_param_in(self, param_file_name) + + module subroutine io_read_in_param(self, param_file_name) !! author: David A. Minton !! !! Read in parameters for the integration @@ -1162,32 +1413,119 @@ module subroutine io_read_param_in(self, param_file_name) ! Internals integer(I4B), parameter :: LUN = 7 !! Unit number of input file integer(I4B) :: ierr = 0 !! Input error code - character(STRMAX) :: error_message !! Error message in UDIO procedure + character(STRMAX) :: errmsg !! Error message in UDIO procedure ! Read in name of parameter file write(*, *) 'Parameter input file is ', trim(adjustl(param_file_name)) write(*, *) ' ' 100 format(A) - open(unit = LUN, file = param_file_name, status = 'old', iostat = ierr) - if (ierr /= 0) then - write(*,*) 'Swiftest error: ', ierr - write(*,*) ' Unable to open file ',trim(adjustl(param_file_name)) - call util_exit(FAILURE) - end if + open(unit = LUN, file = param_file_name, status = 'old', iostat = ierr, err = 667, iomsg = errmsg) !! todo: Currently this procedure does not work in user-defined derived-type input mode !! as the newline characters are ignored in the input file when compiled in ifort. - !read(LUN,'(DT)', iostat= ierr, iomsg = error_message) param - call self%reader(LUN, iotype= "none", v_list = [self%integrator], iostat = ierr, iomsg = error_message) - if (ierr /= 0) then - write(*,*) 'Swiftest error reading ', trim(adjustl(param_file_name)) - write(*,*) ierr,trim(adjustl(error_message)) - call util_exit(FAILURE) - end if + !read(LUN,'(DT)', iostat= ierr, iomsg = errmsg) param + call self%reader(LUN, iotype= "none", v_list = [self%integrator], iostat = ierr, iomsg = errmsg) + if (ierr == 0) return - return - end subroutine io_read_param_in + 667 continue + write(*,*) "Error reading parameter file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_read_in_param + + + module subroutine io_read_in_particle_info(self, iu) + !! author: David A. Minton + !! + !! Reads in particle information object information from an open file unformatted file + implicit none + ! Arguments + class(swiftest_particle_info), intent(inout) :: self !! Particle metadata information object + integer(I4B), intent(in) :: iu !! Open file unit number + ! Internals + character(STRMAX) :: errmsg + + read(iu, err = 667, iomsg = errmsg) self%name + read(iu, err = 667, iomsg = errmsg) self%particle_type + read(iu, err = 667, iomsg = errmsg) self%origin_type + read(iu, err = 667, iomsg = errmsg) self%origin_time + read(iu, err = 667, iomsg = errmsg) self%origin_xh(:) + read(iu, err = 667, iomsg = errmsg) self%origin_vh(:) + + return + + 667 continue + write(*,*) "Error reading particle metadata information from file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_read_in_particle_info + + + module subroutine io_read_particle_info_system(self, param) + !! author: David A. Minton + !! + !! Reads an old particle information file for a restartd run + implicit none + ! Arguments + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + ! Internals + integer(I4B), parameter :: LUN = 22 + integer(I4B) :: i, id, idx + logical :: lmatch + character(STRMAX) :: errmsg + type(swiftest_particle_info), allocatable :: tmpinfo + + open(unit = LUN, file = param%particle_out, status = 'OLD', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + + allocate(tmpinfo, mold=self%cb%info) + + select type(cb => self%cb) + class is (swiftest_cb) + select type(pl => self%pl) + class is (swiftest_pl) + select type(tp => self%tp) + class is (swiftest_tp) + associate(npl => pl%nbody, ntp => tp%nbody) + do + lmatch = .false. + read(LUN, err = 667, iomsg = errmsg, end = 333) id + + if (id == cb%id) then + call cb%info%read_in(LUN) + lmatch = .true. + else + if (npl > 0) then + idx = findloc(pl%id(1:npl), id, dim=1) + if (idx /= 0) then + call pl%info(idx)%read_in(LUN) + lmatch = .true. + end if + end if + if (.not.lmatch .and. ntp > 0) then + idx = findloc(tp%id(1:ntp), id, dim=1) + if (idx /= 0) then + call tp%info(idx)%read_in(LUN) + lmatch = .true. + end if + end if + end if + if (.not.lmatch) then + call tmpinfo%read_in(LUN) + end if + end do + end associate + close(unit = LUN, err = 667, iomsg = errmsg) + end select + end select + end select + + 333 continue + return + + 667 continue + write(*,*) "Error reading particle information file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_read_particle_info_system module subroutine io_toupper(string) @@ -1225,10 +1563,10 @@ module subroutine io_write_discard(self, param) implicit none ! Arguments class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals integer(I4B), parameter :: LUN = 40 - integer(I4B) :: i, ierr + integer(I4B) :: i logical, save :: lfirst = .true. real(DP), dimension(:,:), allocatable :: vh character(*), parameter :: HDRFMT = '(E23.16, 1X, I8, 1X, L1)' @@ -1237,14 +1575,30 @@ module subroutine io_write_discard(self, param) character(*), parameter :: NPLFMT = '(I8)' character(*), parameter :: PLNAMEFMT = '(I8, 2(1X, E23.16))' class(swiftest_body), allocatable :: pltemp + character(len=STRMAX) :: errmsg, out_stat associate(tp_discards => self%tp_discards, nsp => self%tp_discards%nbody, pl => self%pl, npl => self%pl%nbody) + + ! Record the discarded body metadata information to file + if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + call param%nciu%open(param) + call tp_discards%write_particle_info(param%nciu) + call param%nciu%close(param) + end if + + if (param%discard_out == "") return + if (nsp == 0) return - select case(param%out_stat) + if (lfirst) then + out_stat = param%out_stat + else + out_stat = 'APPEND' + end if + select case(out_stat) case('APPEND') - open(unit = LUN, file = param%discard_out, status = 'OLD', position = 'APPEND', form = 'FORMATTED', iostat = ierr) + open(unit = LUN, file = param%discard_out, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) case('NEW', 'REPLACE', 'UNKNOWN') - open(unit = LUN, file = param%discard_out, status = param%out_stat, form = 'FORMATTED', iostat = ierr) + open(unit = LUN, file = param%discard_out, status = param%out_stat, form = 'FORMATTED', err = 667, iomsg = errmsg) case default write(*,*) 'Invalid status code for OUT_STAT: ',trim(adjustl(param%out_stat)) call util_exit(FAILURE) @@ -1254,82 +1608,93 @@ module subroutine io_write_discard(self, param) write(LUN, HDRFMT) param%t, nsp, param%lbig_discard do i = 1, nsp - write(LUN, NAMEFMT) SUB, tp_discards%id(i), tp_discards%status(i) - write(LUN, VECFMT) tp_discards%xh(1, i), tp_discards%xh(2, i), tp_discards%xh(3, i) - write(LUN, VECFMT) tp_discards%vh(1, i), tp_discards%vh(2, i), tp_discards%vh(3, i) + write(LUN, NAMEFMT, err = 667, iomsg = errmsg) SUB, tp_discards%id(i), tp_discards%status(i) + write(LUN, VECFMT, err = 667, iomsg = errmsg) tp_discards%xh(1, i), tp_discards%xh(2, i), tp_discards%xh(3, i) + write(LUN, VECFMT, err = 667, iomsg = errmsg) tp_discards%vh(1, i), tp_discards%vh(2, i), tp_discards%vh(3, i) end do if (param%lbig_discard) then - if (param%lgr) then - allocate(pltemp, source = pl) - call pltemp%pv2v(param) - allocate(vh, source = pltemp%vh) - deallocate(pltemp) - else - allocate(vh, source = pl%vh) - end if + if (param%lgr) then + allocate(pltemp, source = pl) + call pltemp%pv2v(param) + allocate(vh, source = pltemp%vh) + deallocate(pltemp) + else + allocate(vh, source = pl%vh) + end if - write(LUN, NPLFMT) npl - do i = 1, npl - write(LUN, PLNAMEFMT) pl%id(i), pl%Gmass(i), pl%radius(i) - write(LUN, VECFMT) pl%xh(1, i), pl%xh(2, i), pl%xh(3, i) - write(LUN, VECFMT) vh(1, i), vh(2, i), vh(3, i) - end do - deallocate(vh) + write(LUN, NPLFMT) npl + do i = 1, npl + write(LUN, PLNAMEFMT, err = 667, iomsg = errmsg) pl%id(i), pl%Gmass(i), pl%radius(i) + write(LUN, VECFMT, err = 667, iomsg = errmsg) pl%xh(1, i), pl%xh(2, i), pl%xh(3, i) + write(LUN, VECFMT, err = 667, iomsg = errmsg) vh(1, i), vh(2, i), vh(3, i) + end do + deallocate(vh) end if close(LUN) end associate return + + 667 continue + write(*,*) "Error writing discard file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_write_discard - module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & - xh1, xh2, vh1, vh2, enc_out, out_type) - !! author: David A. Minton - !! - !! Write close encounter data to output binary files - !! There is no direct file output from this subroutine - !! - !! Adapted from David E. Kaufmann's Swifter routine: io_write_encounter.f90 - !! Adapted from Hal Levison's Swift routine io_write_encounter.f + module subroutine io_write_encounter(self, pl, encbody, param) implicit none ! Arguments - integer(I4B), intent(in) :: name1, name2 - real(DP), intent(in) :: t, mass1, mass2, radius1, radius2 - real(DP), dimension(:), intent(in) :: xh1, xh2, vh1, vh2 - character(*), intent(in) :: enc_out, out_type + class(swiftest_encounter), intent(in) :: self !! Swiftest encounter list object + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object + class(swiftest_body), intent(in) :: encbody !! Encountering body - Swiftest generic body object (pl or tp) + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters ! Internals - logical , save :: lfirst = .true. - integer(I4B), parameter :: lun = 30 - integer(I4B) :: ierr - integer(I4B), save :: iu = lun + logical , save :: lfirst = .true. + integer(I4B), parameter :: LUN = 30 + integer(I4B) :: k, ierr + character(len=STRMAX) :: errmsg - open(unit = iu, file = enc_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) - if ((ierr /= 0) .and. lfirst) then - open(unit = iu, file = enc_out, status = 'NEW', form = 'UNFORMATTED', iostat = ierr) - end if + if (param%enc_out == "" .or. self%nenc == 0) return + + open(unit = LUN, file = param%enc_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr, iomsg = errmsg) if (ierr /= 0) then - write(*, *) "Swiftest Error:" - write(*, *) " Unable to open binary encounter file" - call util_exit(FAILURE) + if (lfirst) then + open(unit = LUN, file = param%enc_out, status = 'NEW', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + else + goto 667 + end if end if lfirst = .false. - write(iu, iostat = ierr) t - if (ierr < 0) then - write(*, *) "Swiftest Error:" - write(*, *) " Unable to write binary file record" - call util_exit(FAILURE) - end if - write(iu) name1, xh1(1), xh1(2), xh1(3), vh1(1), vh1(2), mass1, radius1 - write(iu) name2, xh2(1), xh2(2), xh2(3), vh2(1), vh2(2), mass2, radius2 - close(unit = iu, iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest Error:" - write(*, *) " Unable to close binary encounter file" - call util_exit(FAILURE) - end if + + associate(ind1 => self%index1, ind2 => self%index2) + select type(encbody) + class is (swiftest_pl) + do k = 1, self%nenc + call io_write_frame_encounter(LUN, self%t(k), & + pl%id(ind1(k)), encbody%id(ind2(k)), & + pl%Gmass(ind1(k)), encbody%Gmass(ind2(k)), & + pl%radius(ind1(k)), encbody%radius(ind2(k)), & + self%x1(:,k), self%x2(:,k), & + self%v1(:,k), self%v2(:,k)) + end do + class is (swiftest_tp) + do k = 1, self%nenc + call io_write_frame_encounter(LUN, self%t(k), & + pl%id(ind1(k)), encbody%id(ind2(k)), & + pl%Gmass(ind1(k)), 0.0_DP, & + pl%radius(ind1(k)), 0.0_DP, & + self%x1(:,k), self%x2(:,k), & + self%v1(:,k), self%v2(:,k)) + end do + end select + end associate + + close(unit = LUN, err = 667, iomsg = errmsg) return + 667 continue + write(*,*) "Error writing encounter file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_write_encounter @@ -1346,48 +1711,53 @@ module subroutine io_write_frame_body(self, iu, param) class(swiftest_body), intent(in) :: self !! Swiftest particle object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + character(len=STRMAX) :: errmsg associate(n => self%nbody) if (n == 0) return - write(iu) self%id(1:n) - !write(iu) self%name(1:n) - select case (param%out_form) - case (EL) - write(iu) self%a(1:n) - write(iu) self%e(1:n) - write(iu) self%inc(1:n) - write(iu) self%capom(1:n) - write(iu) self%omega(1:n) - write(iu) self%capm(1:n) - case (XV) - write(iu) self%xh(1, 1:n) - write(iu) self%xh(2, 1:n) - write(iu) self%xh(3, 1:n) - write(iu) self%vh(1, 1:n) - write(iu) self%vh(2, 1:n) - write(iu) self%vh(3, 1:n) - end select + write(iu, err = 667, iomsg = errmsg) self%id(1:n) + write(iu, err = 667, iomsg = errmsg) self%info(1:n)%name + if ((param%out_form == XV) .or. (param%out_form == XVEL)) then + write(iu, err = 667, iomsg = errmsg) self%xh(1, 1:n) + write(iu, err = 667, iomsg = errmsg) self%xh(2, 1:n) + write(iu, err = 667, iomsg = errmsg) self%xh(3, 1:n) + write(iu, err = 667, iomsg = errmsg) self%vh(1, 1:n) + write(iu, err = 667, iomsg = errmsg) self%vh(2, 1:n) + write(iu, err = 667, iomsg = errmsg) self%vh(3, 1:n) + end if + if ((param%out_form == EL) .or. (param%out_form == XVEL)) then + write(iu, err = 667, iomsg = errmsg) self%a(1:n) + write(iu, err = 667, iomsg = errmsg) self%e(1:n) + write(iu, err = 667, iomsg = errmsg) self%inc(1:n) * RAD2DEG + write(iu, err = 667, iomsg = errmsg) self%capom(1:n) * RAD2DEG + write(iu, err = 667, iomsg = errmsg) self%omega(1:n) * RAD2DEG + write(iu, err = 667, iomsg = errmsg) self%capm(1:n) * RAD2DEG + end if select type(pl => self) class is (swiftest_pl) ! Additional output if the passed polymorphic object is a massive body - write(iu) pl%Gmass(1:n) - if (param%lrhill_present) write(iu) pl%rhill(1:n) - if (param%lclose) write(iu) pl%radius(1:n) + write(iu, err = 667, iomsg = errmsg) pl%Gmass(1:n) + if (param%lrhill_present) write(iu, err = 667, iomsg = errmsg) pl%rhill(1:n) + write(iu, err = 667, iomsg = errmsg) pl%radius(1:n) if (param%lrotation) then - write(iu) pl%Ip(1, 1:n) - write(iu) pl%Ip(2, 1:n) - write(iu) pl%Ip(3, 1:n) - write(iu) pl%rot(1, 1:n) - write(iu) pl%rot(2, 1:n) - write(iu) pl%rot(3, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%Ip(1, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%Ip(2, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%Ip(3, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%rot(1, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%rot(2, 1:n) + write(iu, err = 667, iomsg = errmsg) pl%rot(3, 1:n) end if if (param%ltides) then - write(iu) pl%k2(1:n) - write(iu) pl%Q(1:n) + write(iu, err = 667, iomsg = errmsg) pl%k2(1:n) + write(iu, err = 667, iomsg = errmsg) pl%Q(1:n) end if end select end associate return + 667 continue + write(*,*) "Error writing body frame: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_write_frame_body @@ -1403,33 +1773,68 @@ module subroutine io_write_frame_cb(self, iu, param) class(swiftest_cb), intent(in) :: self !! Swiftest central body object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + character(len=STRMAX) :: errmsg associate(cb => self) - !write(iu) cb%name - write(iu) cb%id - write(iu) cb%Gmass - write(iu) cb%radius - write(iu) cb%j2rp2 - write(iu) cb%j4rp4 + write(iu, err = 667, iomsg = errmsg) cb%id + write(iu, err = 667, iomsg = errmsg) cb%info%name + write(iu, err = 667, iomsg = errmsg) cb%Gmass + write(iu, err = 667, iomsg = errmsg) cb%radius + write(iu, err = 667, iomsg = errmsg) cb%j2rp2 + write(iu, err = 667, iomsg = errmsg) cb%j4rp4 if (param%lrotation) then - write(iu) cb%Ip(1) - write(iu) cb%Ip(2) - write(iu) cb%Ip(3) - write(iu) cb%rot(1) - write(iu) cb%rot(2) - write(iu) cb%rot(3) + write(iu, err = 667, iomsg = errmsg) cb%Ip(1) + write(iu, err = 667, iomsg = errmsg) cb%Ip(2) + write(iu, err = 667, iomsg = errmsg) cb%Ip(3) + write(iu, err = 667, iomsg = errmsg) cb%rot(1) + write(iu, err = 667, iomsg = errmsg) cb%rot(2) + write(iu, err = 667, iomsg = errmsg) cb%rot(3) end if if (param%ltides) then - write(iu) cb%k2 - write(iu) cb%Q + write(iu, err = 667, iomsg = errmsg) cb%k2 + write(iu, err = 667, iomsg = errmsg) cb%Q end if end associate return + 667 continue + write(*,*) "Error writing central body frame: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_write_frame_cb - module subroutine io_write_frame_system(self, iu, param) + module subroutine io_write_frame_encounter(iu, t, id1, id2, Gmass1, Gmass2, radius1, radius2, xh1, xh2, vh1, vh2) + !! author: David A. Minton + !! + !! Write a single frame of close encounter data to output binary files + !! + !! Adapted from David E. Kaufmann's Swifter routine: io_write_encounter.f90 + !! Adapted from Hal Levison's Swift routine io_write_encounter.f + implicit none + ! Arguments + integer(I4B), intent(in) :: iu !! Open file unit number + real(DP), intent(in) :: t !! Time of encounter + integer(I4B), intent(in) :: id1, id2 !! ids of the two encountering bodies + real(DP), intent(in) :: Gmass1, Gmass2 !! G*mass of the two encountering bodies + real(DP), intent(in) :: radius1, radius2 !! Radii of the two encountering bodies + real(DP), dimension(:), intent(in) :: xh1, xh2 !! Heliocentric position vectors of the two encountering bodies + real(DP), dimension(:), intent(in) :: vh1, vh2 !! Heliocentric velocity vectors of the two encountering bodies + ! Internals + character(len=STRMAX) :: errmsg + + write(iu, err = 667, iomsg = errmsg) t + write(iu, err = 667, iomsg = errmsg) id1, xh1(1), xh1(2), xh1(3), vh1(1), vh1(2), Gmass1, radius1 + write(iu, err = 667, iomsg = errmsg) id2, xh2(1), xh2(2), xh2(3), vh2(1), vh2(2), Gmass2, radius2 + + return + 667 continue + write(*,*) "Error writing encounter file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine + + + module subroutine io_write_frame_system(self, param) !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! !! Write a frame (header plus records for each massive body and active test particle) to output binary file @@ -1439,73 +1844,111 @@ module subroutine io_write_frame_system(self, iu, param) !! Adapted from Hal Levison's Swift routine io_write_frame.F implicit none ! Arguments - class(swiftest_nbody_system), intent(in) :: self !! Swiftest system object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals logical, save :: lfirst = .true. !! Flag to determine if this is the first call of this method - integer(I4B) :: ierr !! I/O error code - class(swiftest_cb), allocatable :: cb !! Temporary local version of pl structure used for non-destructive conversions class(swiftest_pl), allocatable :: pl !! Temporary local version of pl structure used for non-destructive conversions class(swiftest_tp), allocatable :: tp !! Temporary local version of pl structure used for non-destructive conversions + character(len=STRMAX) :: errmsg + integer(I4B) :: iu = BINUNIT !! Unit number for the output file to write frame to + logical :: fileExists + + if (.not.lfirst .and. param%lenergy) call self%conservation_report(param, lterminal=.true.) allocate(cb, source = self%cb) allocate(pl, source = self%pl) allocate(tp, source = self%tp) iu = BINUNIT - - if (lfirst) then - select case(param%out_stat) - case('APPEND') - open(unit = iu, file = param%outfile, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) - case('NEW', 'REPLACE', 'UNKNOWN') - open(unit = iu, file = param%outfile, status = param%out_stat, form = 'UNFORMATTED', iostat = ierr) - case default - write(*,*) 'Invalid status code for OUT_STAT: ',trim(adjustl(param%out_stat)) - call util_exit(FAILURE) - end select - if (ierr /= 0) then - write(*, *) "Swiftest error: io_write_frame_system - first", ierr - write(*, *) " Binary output file " // trim(adjustl(param%outfile)) // " already exists or cannot be accessed" - write(*, *) " OUT_STAT: " // trim(adjustl(param%out_stat)) - call util_exit(FAILURE) + + if ((param%out_type == REAL4_TYPE) .or. (param%out_type == REAL8_TYPE)) then + if (lfirst) then + select case(param%out_stat) + case('APPEND') + open(unit = iu, file = param%outfile, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', err = 667, iomsg = errmsg) + case('NEW', 'REPLACE', 'UNKNOWN') + open(unit = iu, file = param%outfile, status = param%out_stat, form = 'UNFORMATTED', err = 667, iomsg = errmsg) + case default + write(*,*) 'Invalid status code for OUT_STAT: ',trim(adjustl(param%out_stat)) + call util_exit(FAILURE) + end select + + lfirst = .false. + else + open(unit = iu, file = param%outfile, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', err = 667, iomsg = errmsg) end if - lfirst = .false. - else - open(unit = iu, file = param%outfile, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest error: io_write_frame_system" - write(*, *) " Unable to open binary output file for APPEND" - call util_exit(FAILURE) + else if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + + if (lfirst) then + inquire(file=param%outfile, exist=fileExists) + + select case(param%out_stat) + case('APPEND') + if (.not.fileExists) then + errmsg = param%outfile // " not found! You must specify OUT_STAT = NEW, REPLACE, or UNKNOWN" + goto 667 + end if + case('NEW') + if (fileExists) then + errmsg = param%outfile // " Alread Exists! You must specify OUT_STAT = OLD, REPLACE, or UNKNOWN" + goto 667 + end if + case('REPLACE', 'UNKNOWN') + if (fileExists) then + open(file=param%outfile, unit=iu, status='OLD') + close (unit=BINUNIT, status="delete") + end if + end select + + select case(param%out_stat) + case('APPEND') + call param%nciu%open(param) + case('NEW', 'REPLACE', 'UNKNOWN') + call param%nciu%initialize(param) + call param%nciu%close(param) + call param%nciu%open(param) + end select + lfirst = .false. + else + call param%nciu%open(param) end if end if - call io_write_hdr(iu, param%t, pl%nbody, tp%nbody, param%out_form, param%out_type) if (param%lgr) then call pl%pv2v(param) call tp%pv2v(param) end if - if (param%out_form == EL) then ! Do an orbital element conversion prior to writing out the frame, as we have access to the central body here + if ((param%out_form == EL) .or. (param%out_form == XVEL)) then ! Do an orbital element conversion prior to writing out the frame, as we have access to the central body here call pl%xv2el(cb) call tp%xv2el(cb) end if ! Write out each data type frame - call cb%write_frame(iu, param) - call pl%write_frame(iu, param) - call tp%write_frame(iu, param) - - deallocate(cb, pl, tp) - - close(iu) + if ((param%out_type == REAL4_TYPE) .or. (param%out_type == REAL8_TYPE)) then + call self%write_hdr(iu, param) + call cb%write_frame(iu, param) + call pl%write_frame(iu, param) + call tp%write_frame(iu, param) + close(iu, err = 667, iomsg = errmsg) + else if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + call self%write_hdr(param%nciu, param) + call cb%write_frame(param%nciu, param) + call pl%write_frame(param%nciu, param) + call tp%write_frame(param%nciu, param) + call param%nciu%close(param) + end if return + + 667 continue + write(*,*) "Error writing system frame: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine io_write_frame_system - subroutine io_write_hdr(iu, t, npl, ntp, out_form, out_type) + module subroutine io_write_hdr_system(self, iu, param) ! t, npl, ntp, out_form, out_type) !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! !! Write frame header to output binary file @@ -1514,36 +1957,27 @@ subroutine io_write_hdr(iu, t, npl, ntp, out_form, out_type) !! Adapted from Hal Levison's Swift routine io_write_hdr.F implicit none ! Arguments - integer(I4B), intent(in) :: iu !! Output file unit number - real(DP), intent(in) :: t !! Current time of simulation - integer(I4B), intent(in) :: npl !! Number of massive bodies - integer(I4B), intent(in) :: ntp !! Number of test particles - character(*), intent(in) :: out_form !! Output format type ("EL" or "XV") - character(*), intent(in) :: out_type !! Output file format type (REAL4, REAL8 - see swiftest module for symbolic name definitions) + class(swiftest_nbody_system), intent(in) :: self !! Swiftest nbody system object + integer(I4B), intent(inout) :: iu !! Output file unit number + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters ! Internals - integer(I4B) :: ierr !! Error code + character(len=STRMAX) :: errmsg - select case (out_type) - case (REAL4_TYPE,SWIFTER_REAL4_TYPE) - write(iu, iostat = ierr) real(t, kind=SP) - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " Unable to write binary file header" - call util_exit(FAILURE) - end if - case (REAL8_TYPE,SWIFTER_REAL8_TYPE) - write(iu, iostat = ierr) t - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " Unable to write binary file header" - call util_exit(FAILURE) - end if + select case (param%out_type) + case (REAL4_TYPE) + write(iu, err = 667, iomsg = errmsg) real(param%t, kind=SP) + case (REAL8_TYPE) + write(iu, err = 667, iomsg = errmsg) param%t end select - write(iu, iostat = ierr) npl - write(iu, iostat = ierr) ntp - write(iu, iostat = ierr) out_form + write(iu, err = 667, iomsg = errmsg) self%pl%nbody + write(iu, err = 667, iomsg = errmsg) self%tp%nbody + write(iu, err = 667, iomsg = errmsg) param%out_form return - end subroutine io_write_hdr + + 667 continue + write(*,*) "Error writing header: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) + end subroutine io_write_hdr_system end submodule s_io diff --git a/src/kick/kick.f90 b/src/kick/kick.f90 index 3945a91d0..5c57918e2 100644 --- a/src/kick/kick.f90 +++ b/src/kick/kick.f90 @@ -2,7 +2,7 @@ use swiftest contains - module pure subroutine kick_getacch_int_pl(self) + module subroutine kick_getacch_int_pl(self) !! author: David A. Minton !! !! Compute direct cross (third) term heliocentric accelerations of massive bodies @@ -12,26 +12,8 @@ module pure subroutine kick_getacch_int_pl(self) implicit none ! Arguments class(swiftest_pl), intent(inout) :: self - ! Internals - integer(I4B) :: k - real(DP) :: rji2, irij3, faci, facj - real(DP), dimension(NDIM) :: dx - - associate(pl => self, npl => self%nbody, nplpl => self%nplpl) - do k = 1, nplpl - associate(i => pl%k_plpl(1, k), j => pl%k_plpl(2, k)) - if (pl%lmask(i) .and. pl%lmask(j)) then - dx(:) = pl%xh(:, j) - pl%xh(:, i) - rji2 = dot_product(dx(:), dx(:)) - irij3 = 1.0_DP / (rji2 * sqrt(rji2)) - faci = pl%Gmass(i) * irij3 - facj = pl%Gmass(j) * irij3 - pl%ah(:, i) = pl%ah(:, i) + facj * dx(:) - pl%ah(:, j) = pl%ah(:, j) - faci * dx(:) - end if - end associate - end do - end associate + + call kick_getacch_int_all_pl(self%nbody, self%nplpl, self%k_plpl, self%xh, self%Gmass, self%radius, self%ah) return end subroutine kick_getacch_int_pl @@ -52,21 +34,127 @@ module pure subroutine kick_getacch_int_tp(self, GMpl, xhp, npl) integer(I4B), intent(in) :: npl !! Number of active massive bodies ! Internals integer(I4B) :: i, j - real(DP) :: rji2, irij3, fac, r2 - real(DP), dimension(NDIM) :: dx + + if ((self%nbody == 0) .or. (npl == 0)) return associate(tp => self, ntp => self%nbody) - do concurrent(i = 1:ntp, tp%lmask(i)) - do j = 1, npl - dx(:) = tp%xh(:,i) - xhp(:, j) - r2 = dot_product(dx(:), dx(:)) - fac = GMpl(j) / (r2 * sqrt(r2)) - tp%ah(:, i) = tp%ah(:, i) - fac * dx(:) - end do + do i = 1, ntp + if (tp%lmask(i)) then + do j = 1, npl + block + real(DP) :: rji2 + real(DP) :: xr, yr, zr + xr = tp%xh(1, i) - xhp(1, j) + yr = tp%xh(2, i) - xhp(1, j) + zr = tp%xh(3, i) - xhp(1, j) + rji2 = xr**2 + yr**2 + zr**2 + call kick_getacch_int_one_tp(rji2, xr, yr, zr, GMpl(i), tp%ah(1,i), tp%ah(2,i), tp%ah(3,i)) + end block + end do + end if end do end associate return end subroutine kick_getacch_int_tp + + module subroutine kick_getacch_int_all_pl(npl, nplpl, k_plpl, x, Gmass, radius, acc) + !! author: David A. Minton + !! + !! Compute direct cross (third) term heliocentric accelerations for massive bodies, with parallelization + !! + !! Adapted from Hal Levison's Swift routine getacch_ah3.f + !! Adapted from David E. Kaufmann's Swifter routine whm_kick_getacch_ah3.f90 and helio_kick_getacch_int.f9 + implicit none + integer(I4B), intent(in) :: npl !! Number of massive bodies + integer(I8B), intent(in) :: nplpl !! Number of massive body interactions to compute + integer(I4B), dimension(:,:), intent(in) :: k_plpl !! Array of interaction pair indices (flattened upper triangular matrix) + real(DP), dimension(:,:), intent(in) :: x !! Position vector array + real(DP), dimension(:), intent(in) :: Gmass !! Array of massive body G*mass + real(DP), dimension(:), intent(in) :: radius !! Array of massive body radii + real(DP), dimension(:,:), intent(inout) :: acc !! Acceleration vector array + ! Internals + integer(I8B) :: k + real(DP) :: rji2, rlim2 + real(DP) :: xr, yr, zr + integer(I4B) :: i, j + real(DP), dimension(NDIM,npl) :: ahi, ahj + + ahi(:,:) = 0.0_DP + ahj(:,:) = 0.0_DP + !$omp parallel do default(private)& + !$omp shared(nplpl, k_plpl, x, Gmass, radius) & + !$omp reduction(+:ahi) & + !$omp reduction(-:ahj) + do k = 1_I8B, nplpl + i = k_plpl(1,k) + j = k_plpl(2,k) + xr = x(1, j) - x(1, i) + yr = x(2, j) - x(2, i) + zr = x(3, j) - x(3, i) + rji2 = xr**2 + yr**2 + zr**2 + rlim2 = (radius(i) + radius(j))**2 + if (rji2 > rlim2) call kick_getacch_int_one_pl(rji2, xr, yr, zr, Gmass(i), Gmass(j), ahi(1,i), ahi(2,i), ahi(3,i), ahj(1,j), ahj(2,j), ahj(3,j)) + end do + !$omp end parallel do + + acc(:,1:npl) = acc(:,1:npl) + ahi(:,1:npl) + ahj(:,1:npl) + return + end subroutine kick_getacch_int_all_pl + + + module pure subroutine kick_getacch_int_one_pl(rji2, xr, yr, zr, Gmi, Gmj, axi, ayi, azi, axj, ayj, azj) + !! author: David A. Minton + !! + !! Compute direct cross (third) term heliocentric accelerations for a single pair of massive bodies + !! + !! Adapted from Hal Levison's Swift routine getacch_ah3.f + !! Adapted from David E. Kaufmann's Swifter routine whm_kick_getacch_ah3.f90 and helio_kick_getacch_int.f9 + implicit none + real(DP), intent(in) :: rji2 !! Square of distance between the two bodies + real(DP), intent(in) :: xr, yr, zr !! Distances between the two bodies in x, y, and z directions + real(DP), intent(in) :: Gmi !! G*mass of body i + real(DP), intent(in) :: Gmj !! G*mass of body j + real(DP), intent(inout) :: axi, ayi, azi !! Acceleration vector components of body i + real(DP), intent(inout) :: axj, ayj, azj !! Acceleration vector components of body j + ! Internals + real(DP) :: faci, facj, irij3 + + irij3 = 1.0_DP / (rji2 * sqrt(rji2)) + faci = Gmi * irij3 + facj = Gmj * irij3 + axi = axi + facj * xr + ayi = ayi + facj * yr + azi = azi + facj * zr + axj = axj - faci * xr + ayj = ayj - faci * yr + azj = azj - faci * zr + + return + end subroutine kick_getacch_int_one_pl + + + module pure subroutine kick_getacch_int_one_tp(rji2, xr, yr, zr, GMpl, ax, ay, az) + !! author: David A. Minton + !! + !! Compute direct cross (third) term heliocentric accelerations of a single test particle massive body pair. + !! + !! Adapted from Hal Levison's Swift routine getacch_ah3_tp.f + !! Adapted from David E. Kaufmann's Swifter routine whm_kick_getacch_ah3.f90 and helio_kick_getacch_int_tp.f90 + implicit none + real(DP), intent(in) :: rji2 !! Square of distance between the test particle and massive body + real(DP), intent(in) :: xr, yr, zr !! Distances between the two bodies in x, y, and z directions + real(DP), intent(in) :: Gmpl !! G*mass of massive body + real(DP), intent(inout) :: ax, ay, az !! Acceleration vector components of test particle + ! Internals + real(DP) :: fac + + fac = GMpl / (rji2 * sqrt(rji2)) + ax = ax - fac * xr + ay = ay - fac * yr + az = az - fac * zr + return + end subroutine kick_getacch_int_one_tp + end submodule s_kick diff --git a/src/main/swiftest_driver.f90 b/src/main/swiftest_driver.f90 index 5e28452e0..b4260f115 100644 --- a/src/main/swiftest_driver.f90 +++ b/src/main/swiftest_driver.f90 @@ -17,8 +17,10 @@ program swiftest_driver integer(I8B) :: iloop !! Loop counter integer(I8B) :: idump !! Dump cadence counter integer(I8B) :: iout !! Output cadence counter + integer(I8B) :: ioutput_t0 !! The output frame counter at time 0 integer(I8B) :: nloops !! Number of steps to take in the simulation - integer(I4B) :: iu !! Unit number of binary file + real(DP) :: old_t_final = 0.0_DP !! Output time at which writing should start, in order to prevent duplicate lines being written for restarts + type(walltimer) :: timer !! Object used for computing elapsed wall time ierr = io_get_args(integrator, param_file_name) if (ierr /= 0) then @@ -35,23 +37,32 @@ program swiftest_driver param%integrator = integrator call setup_construct_system(nbody_system, param) - call param%read_from_file(param_file_name) + call param%read_in(param_file_name) associate(t => param%t, & t0 => param%t0, & dt => param%dt, & tstop => param%tstop, & istep_out => param%istep_out, & - istep_dump => param%istep_dump) + istep_dump => param%istep_dump, & + ioutput => param%ioutput) call nbody_system%initialize(param) t = t0 iloop = 0 iout = istep_out idump = istep_dump - nloops = ceiling(tstop / dt, kind=I8B) - if (istep_out > 0) call nbody_system%write_frame(iu, param) - call nbody_system%dump(param) + nloops = ceiling((tstop - t0) / dt, kind=I8B) + ioutput_t0 = int(t0 / dt / istep_out, kind=I8B) + ioutput = ioutput_t0 + ! Prevent duplicate frames from being written if this is a restarted run + if ((param%lrestart) .and. ((param%out_type == REAL8_TYPE) .or. param%out_type == REAL4_TYPE)) then + old_t_final = nbody_system%get_old_t_final(param) + else + old_t_final = t0 + if (istep_out > 0) call nbody_system%write_frame(param) + call nbody_system%dump(param) + end if !> Define the maximum number of threads nthreads = 1 ! In the *serial* case @@ -59,6 +70,7 @@ program swiftest_driver !$ write(*,'(a)') ' OpenMP parameters:' !$ write(*,'(a)') ' ------------------' !$ write(*,'(a,i3,/)') ' Number of threads = ', nthreads + call timer%reset() write(*, *) " *************** Main Loop *************** " do iloop = 1, nloops !> Step the system forward in time @@ -73,7 +85,10 @@ program swiftest_driver if (istep_out > 0) then iout = iout - 1 if (iout == 0) then - call nbody_system%write_frame(iu, param) + ioutput = ioutput_t0 + iloop / istep_out + call timer%finish(nsubsteps=istep_out, message="Integration steps:") + if (t > old_t_final) call nbody_system%write_frame(param) + call timer%finish(nsubsteps=1, message="File I/O: ") iout = istep_out end if end if diff --git a/src/modules/fraggle_classes.f90 b/src/modules/fraggle_classes.f90 new file mode 100644 index 000000000..5a8a4a392 --- /dev/null +++ b/src/modules/fraggle_classes.f90 @@ -0,0 +1,282 @@ +module fraggle_classes + !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott + !! + !! Definition of classes and methods specific to Fraggel: The Fragment Generation Model + use swiftest_globals + use swiftest_classes, only : swiftest_parameters, swiftest_nbody_system, swiftest_cb, swiftest_pl + implicit none + public + + integer(I4B), parameter :: FRAGGLE_NMASS_DIST = 3 !! Number of mass bins returned by the regime calculation (largest fragment, second largest, and remainder) + character(len=*), parameter :: FRAGGLE_LOG_OUT = "fraggle.log" !! Name of log file for Fraggle diagnostic information + integer(I4B), parameter :: FRAGGLE_LOG_UNIT = 76 !! Unit number for Fraggle log file + + !******************************************************************************************************************************** + ! fraggle_colliders class definitions and method interfaces + !******************************************************************************************************************************* + !> Class definition for the variables that describe the bodies involved in the collision + type :: fraggle_colliders + integer(I4B) :: ncoll !! Number of bodies involved in the collision + integer(I4B), dimension(:), allocatable :: idx !! Index of bodies involved in the collision + real(DP), dimension(NDIM,2) :: xb !! Two-body equivalent position vectors of the collider bodies prior to collision + real(DP), dimension(NDIM,2) :: vb !! Two-body equivalent velocity vectors of the collider bodies prior to collision + real(DP), dimension(NDIM,2) :: rot !! Two-body equivalent principal axes moments of inertia the collider bodies prior to collision + real(DP), dimension(NDIM,2) :: L_spin !! Two-body equivalent spin angular momentum vectors of the collider bodies prior to collision + real(DP), dimension(NDIM,2) :: L_orbit !! Two-body equivalent orbital angular momentum vectors of the collider bodies prior to collision + real(DP), dimension(NDIM,2) :: Ip !! Two-body equivalent principal axes moments of inertia the collider bodies prior to collision + real(DP), dimension(2) :: mass !! Two-body equivalent mass of the collider bodies prior to the collision + real(DP), dimension(2) :: radius !! Two-body equivalent radii of the collider bodies prior to the collision + contains + procedure :: regime => fraggle_regime_colliders !! Determine which fragmentation regime the set of colliders will be + end type fraggle_colliders + + !******************************************************************************************************************************** + ! fraggle_fragments class definitions and method interfaces + !******************************************************************************************************************************* + !> Class definition for the variables that describe a collection of fragments by Fraggle barycentric coordinates + type, extends(swiftest_pl) :: fraggle_fragments + real(DP) :: mtot !! Total mass of fragments + real(DP) :: Qloss !! Energy lost during the collision + real(DP), dimension(FRAGGLE_NMASS_DIST) :: mass_dist !! Distribution of fragment mass determined by the regime calculation (largest fragment, second largest, and remainder) + integer(I4B) :: regime !! Collresolve regime code for this collision + + ! Values in a coordinate frame centered on the collider barycenter and collisional system unit vectors (these are used internally by the fragment generation subroutine) + real(DP), dimension(NDIM) :: xbcom !! Center of mass position vector of the collider system in system barycentric coordinates + real(DP), dimension(NDIM) :: vbcom !! Velocity vector of the center of mass of the collider system in system barycentric coordinates + real(DP), dimension(NDIM) :: x_coll_unit !! x-direction unit vector of collisional system + real(DP), dimension(NDIM) :: y_coll_unit !! y-direction unit vector of collisional system + real(DP), dimension(NDIM) :: z_coll_unit !! z-direction unit vector of collisional system + real(DP), dimension(:,:), allocatable :: x_coll !! Array of fragment position vectors in the collisional coordinate frame + real(DP), dimension(:,:), allocatable :: v_coll !! Array of fragment velocity vectors in the collisional coordinate frame + real(DP), dimension(:,:), allocatable :: v_r_unit !! Array of radial direction unit vectors of individual fragments in the collisional coordinate frame + real(DP), dimension(:,:), allocatable :: v_t_unit !! Array of tangential direction unit vectors of individual fragments in the collisional coordinate frame + real(DP), dimension(:,:), allocatable :: v_n_unit !! Array of normal direction unit vectors of individual fragments in the collisional coordinate frame + real(DP), dimension(:), allocatable :: rmag !! Array of radial distance magnitudes of individual fragments in the collisional coordinate frame + real(DP), dimension(:), allocatable :: rotmag !! Array of rotation magnitudes of individual fragments + real(DP), dimension(:), allocatable :: v_r_mag !! Array of radial direction velocity magnitudes of individual fragments + real(DP), dimension(:), allocatable :: v_t_mag !! Array of tangential direction velocity magnitudes of individual fragments + + ! Energy and momentum book-keeping variables that characterize the whole system of fragments + real(DP) :: ke_orbit !! Current orbital kinetic energy of the system of fragments in the collisional frame + real(DP) :: ke_spin !! Current spin kinetic energy of the system of fragments in the collisional frame + real(DP), dimension(NDIM) :: L_orbit !! Current orbital angular momentum of the system of fragments in the collisional frame + real(DP), dimension(NDIM) :: L_spin !! Current spin angular momentum of the system of fragments in the collisional frame + real(DP) :: ke_budget !! Total kinetic energy budget for the system of fragmens in the collisional frame + real(DP), dimension(NDIM) :: L_budget !! Total angular momentum budget for the system of fragmens in the collisional frame + + ! For the following variables, "before" refers to the *entire* n-body system in its pre-collisional state and "after" refers to the system in its post-collisional state + real(DP), dimension(NDIM) :: Lorbit_before, Lorbit_after !! Before/after orbital angular momentum + real(DP), dimension(NDIM) :: Lspin_before, Lspin_after !! Before/after spin angular momentum + real(DP), dimension(NDIM) :: Ltot_before, Ltot_after !! Before/after total system angular momentum + real(DP) :: ke_orbit_before, ke_orbit_after !! Before/after orbital kinetic energy + real(DP) :: ke_spin_before, ke_spin_after !! Before/after spin kinetic energy + real(DP) :: pe_before, pe_after !! Before/after potential energy + real(DP) :: Etot_before, Etot_after !! Before/after total system energy + + ! Scale factors used to scale dimensioned quantities to a more "natural" system where important quantities (like kinetic energy, momentum) are of order ~1 + real(DP) :: dscale !! Distance dimension scale factor + real(DP) :: mscale !! Mass scale factor + real(DP) :: tscale !! Time scale factor + real(DP) :: vscale !! Velocity scale factor (a convenience unit that is derived from dscale and tscale) + real(DP) :: Escale !! Energy scale factor (a convenience unit that is derived from dscale, tscale, and mscale) + real(DP) :: Lscale !! Angular momentum scale factor (a convenience unit that is derived from dscale, tscale, and mscale) + contains + procedure :: generate_fragments => fraggle_generate_fragments !! Generates a system of fragments in barycentric coordinates that conserves energy and momentum. + procedure :: accel => fraggle_placeholder_accel !! Placeholder subroutine to fulfill requirement for an accel method + procedure :: kick => fraggle_placeholder_kick !! Placeholder subroutine to fulfill requirement for a kick method + procedure :: step => fraggle_placeholder_step !! Placeholder subroutine to fulfill requirement for a step method + procedure :: set_budgets => fraggle_set_budgets_fragments !! Sets the energy and momentum budgets of the fragments based on the collider value + procedure :: set_coordinate_system => fraggle_set_coordinate_system !! Defines the collisional coordinate system, including the unit vectors of both the system and individual fragments. + procedure :: set_mass_dist => fraggle_set_mass_dist_fragments !! Sets the distribution of mass among the fragments depending on the regime type + procedure :: set_natural_scale => fraggle_set_natural_scale_factors !! Scales dimenional quantities to ~O(1) with respect to the collisional system. + procedure :: set_original_scale => fraggle_set_original_scale_factors !! Restores dimenional quantities back to the original system units + procedure :: setup => fraggle_setup_fragments !! Allocates arrays for n fragments in a Fraggle system. Passing n = 0 deallocates all arrays. + procedure :: reset => fraggle_setup_reset_fragments !! Resets all position and velocity-dependent fragment quantities in order to do a fresh calculation (does not reset mass, radius, or other values that get set prior to the call to fraggle_generate) + procedure :: get_ang_mtm => fraggle_util_ang_mtm !! Calcualtes the current angular momentum of the fragments + procedure :: get_energy_and_momentum => fraggle_util_get_energy_momentum !! Calculates total system energy in either the pre-collision outcome state (lbefore = .true.) or the post-collision outcome state (lbefore = .false.) + procedure :: restructure => fraggle_util_restructure !! Restructure the inputs after a failed attempt failed to find a set of positions and velocities that satisfy the energy and momentum constraints + end type fraggle_fragments + + interface + module subroutine fraggle_generate_fragments(self, colliders, system, param, lfailure) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object containing the two-body equivalent values of the colliding bodies + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + logical, intent(out) :: lfailure !! Answers the question: Should this have been a merger instead? + end subroutine fraggle_generate_fragments + + module subroutine fraggle_io_log_generate(frag) + implicit none + class(fraggle_fragments), intent(in) :: frag + end subroutine fraggle_io_log_generate + + module subroutine fraggle_io_log_one_message(message) + implicit none + character(len=*), intent(in) :: message + character(STRMAX) :: errmsg + end subroutine fraggle_io_log_one_message + + module subroutine fraggle_io_log_pl(pl, param) + implicit none + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object (only the new bodies generated in a collision) + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + end subroutine fraggle_io_log_pl + + module subroutine fraggle_io_log_regime(colliders, frag) + implicit none + class(fraggle_colliders), intent(in) :: colliders + class(fraggle_fragments), intent(in) :: frag + end subroutine fraggle_io_log_regime + + module subroutine fraggle_io_log_start(param) + implicit none + class(swiftest_parameters), intent(in) :: param + end subroutine fraggle_io_log_start + + !> The following interfaces are placeholders intended to satisfy the required abstract methods given by the parent class + module subroutine fraggle_placeholder_accel(self, system, param, t, lbeg) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Current simulation time + logical, intent(in) :: lbeg !! Optional argument that determines whether or not this is the beginning or end of the step + end subroutine fraggle_placeholder_accel + + module subroutine fraggle_placeholder_kick(self, system, param, t, dt, lbeg) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system objec + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Current time + real(DP), intent(in) :: dt !! Stepsize + logical, intent(in) :: lbeg !! Logical flag indicating whether this is the beginning of the half step or not. + end subroutine fraggle_placeholder_kick + + module subroutine fraggle_placeholder_step(self, system, param, t, dt) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(inout) :: self !! Helio massive body particle object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nboody system + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! Current simulation time + real(DP), intent(in) :: dt !! Stepsiz + end subroutine fraggle_placeholder_step + + module subroutine fraggle_regime_colliders(self, frag, system, param) + implicit none + class(fraggle_colliders), intent(inout) :: self !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragment system object + class(swiftest_nbody_system), intent(in) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current Swiftest run configuration parameters + end subroutine fraggle_regime_colliders + + module subroutine fraggle_set_budgets_fragments(self, colliders) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + end subroutine fraggle_set_budgets_fragments + + module subroutine fraggle_set_coordinate_system(self, colliders) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + end subroutine fraggle_set_coordinate_system + + module subroutine fraggle_set_mass_dist_fragments(self, colliders, param) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + class(swiftest_parameters), intent(in) :: param !! Current Swiftest run configuration parameters + end subroutine fraggle_set_mass_dist_fragments + + module subroutine fraggle_set_natural_scale_factors(self, colliders) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + end subroutine fraggle_set_natural_scale_factors + + module subroutine fraggle_set_original_scale_factors(self, colliders) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + end subroutine fraggle_set_original_scale_factors + + module subroutine fraggle_setup_fragments(self, n, param) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + integer(I4B), intent(in) :: n !! Number of fragments + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + end subroutine fraggle_setup_fragments + + module subroutine fraggle_setup_reset_fragments(self) + implicit none + class(fraggle_fragments), intent(inout) :: self + end subroutine fraggle_setup_reset_fragments + + module subroutine fraggle_util_add_fragments_to_system(frag, colliders, system, param) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(in) :: frag !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + end subroutine fraggle_util_add_fragments_to_system + + module subroutine fraggle_util_ang_mtm(self) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + end subroutine fraggle_util_ang_mtm + + module subroutine fraggle_util_construct_temporary_system(frag, system, param, tmpsys, tmpparam) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(in) :: frag !! Fraggle fragment system object + class(swiftest_nbody_system), intent(in) :: system !! Original swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + class(swiftest_nbody_system), allocatable, intent(out) :: tmpsys !! Output temporary swiftest nbody system object + class(swiftest_parameters), allocatable, intent(out) :: tmpparam !! Output temporary configuration run parameters + end subroutine fraggle_util_construct_temporary_system + + module subroutine fraggle_util_get_energy_momentum(self, colliders, system, param, lbefore) + use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle collider system object + class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object + class(swiftest_parameters), intent(in) :: param !! Current swiftest run configuration parameters + logical, intent(in) :: lbefore !! Flag indicating that this the "before" state of the system, with colliders included and fragments excluded or vice versa + end subroutine fraggle_util_get_energy_momentum + + module subroutine fraggle_util_restructure(self, colliders, try, f_spin, r_max_start) + implicit none + class(fraggle_fragments), intent(inout) :: self !! Fraggle fragment system object + class(fraggle_colliders), intent(in) :: colliders !! Fraggle collider system object + integer(I4B), intent(in) :: try !! The current number of times Fraggle has tried to find a solution + real(DP), intent(inout) :: f_spin !! Fraction of energy/momentum that goes into spin. This decreases ater a failed attempt + real(DP), intent(inout) :: r_max_start !! The maximum radial distance that the position calculation starts with. This increases after a failed attempt + end subroutine fraggle_util_restructure + + module subroutine fraggle_util_shift_vector_to_origin(m_frag, vec_frag) + implicit none + real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses + real(DP), dimension(:,:), intent(inout) :: vec_frag !! Fragment positions or velocities in the center of mass frame + end subroutine + + module function fraggle_util_vmag_to_vb(v_r_mag, v_r_unit, v_t_mag, v_t_unit, m_frag, vcom) result(vb) + implicit none + real(DP), dimension(:), intent(in) :: v_r_mag !! Unknown radial component of fragment velocity vector + real(DP), dimension(:), intent(in) :: v_t_mag !! Tangential component of velocity vector set previously by angular momentum constraint + real(DP), dimension(:,:), intent(in) :: v_r_unit, v_t_unit !! Radial and tangential unit vectors for each fragment + real(DP), dimension(:), intent(in) :: m_frag !! Fragment masses + real(DP), dimension(:), intent(in) :: vcom !! Barycentric velocity of collisional system center of mass + real(DP), dimension(:,:), allocatable :: vb + end function fraggle_util_vmag_to_vb + end interface + +end module fraggle_classes \ No newline at end of file diff --git a/src/modules/helio_classes.f90 b/src/modules/helio_classes.f90 index 89f4aa055..1c93bdf6b 100644 --- a/src/modules/helio_classes.f90 +++ b/src/modules/helio_classes.f90 @@ -2,7 +2,7 @@ module helio_classes !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! !! Definition of classes and methods specific to the Democratic Heliocentric Method - !! Adapted from David E. Kaufmann's Swifter routine: helio.f90 + !! Adapted from David E. Kaufmann's Swifter routine: module_helio.f90 use swiftest_globals use swiftest_classes, only : swiftest_cb, swiftest_pl, swiftest_tp, swiftest_nbody_system use whm_classes, only : whm_nbody_system @@ -15,7 +15,8 @@ module helio_classes !******************************************************************************************************************************** type, extends(whm_nbody_system) :: helio_nbody_system contains - procedure :: step => helio_step_system !! Advance the Helio nbody system forward in time by one step + procedure :: step => helio_step_system !! Advance the Helio nbody system forward in time by one step + procedure :: initialize => helio_setup_initialize_system !! Performs Helio-specific initilization steps, including converting to DH coordinates end type helio_nbody_system !******************************************************************************************************************************** @@ -35,8 +36,6 @@ module helio_classes !! Helio massive body particle class type, extends(swiftest_pl) :: helio_pl contains - procedure :: vh2vb => helio_coord_vh2vb_pl !! Convert massive bodies from heliocentric to barycentric coordinates (velocity only) - procedure :: vb2vh => helio_coord_vb2vh_pl !! Convert massive bodies from barycentric to heliocentric coordinates (velocity only) procedure :: drift => helio_drift_pl !! Method for Danby drift in Democratic Heliocentric coordinates procedure :: lindrift => helio_drift_linear_pl !! Method for linear drift of massive bodies due to barycentric momentum of Sun procedure :: accel_gr => helio_gr_kick_getacch_pl !! Acceleration term arising from the post-Newtonian correction @@ -53,8 +52,6 @@ module helio_classes !! Helio test particle class type, extends(swiftest_tp) :: helio_tp contains - procedure :: vh2vb => helio_coord_vh2vb_tp !! Convert test particles from heliocentric to barycentric coordinates (velocity only) - procedure :: vb2vh => helio_coord_vb2vh_tp !! Convert test particles from barycentric to heliocentric coordinates (velocity only) procedure :: lindrift => helio_drift_linear_tp !! Method for linear drift of massive bodies due to barycentric momentum of Sun procedure :: drift => helio_drift_tp !! Method for Danby drift in Democratic Heliocentric coordinates procedure :: accel_gr => helio_gr_kick_getacch_tp !! Acceleration term arising from the post-Newtonian correction @@ -65,32 +62,6 @@ module helio_classes end type helio_tp interface - module subroutine helio_coord_vb2vh_pl(self, cb) - use swiftest_classes, only : swiftest_cb - implicit none - class(helio_pl), intent(inout) :: self !! Helio massive body object - class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - end subroutine helio_coord_vb2vh_pl - - module subroutine helio_coord_vb2vh_tp(self, vbcb) - implicit none - class(helio_tp), intent(inout) :: self !! Helio massive body object - real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body - end subroutine helio_coord_vb2vh_tp - - module subroutine helio_coord_vh2vb_pl(self, cb) - use swiftest_classes, only : swiftest_cb - implicit none - class(helio_pl), intent(inout) :: self !! Helio massive body object - class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - end subroutine helio_coord_vh2vb_pl - - module subroutine helio_coord_vh2vb_tp(self, vbcb) - implicit none - class(helio_tp), intent(inout) :: self !! Helio massive body object - real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body - end subroutine helio_coord_vh2vb_tp - module subroutine helio_drift_body(self, system, param, dt) use swiftest_classes, only : swiftest_body, swiftest_nbody_system, swiftest_parameters implicit none @@ -206,6 +177,13 @@ module subroutine helio_kick_vb_tp(self, system, param, t, dt, lbeg) logical, intent(in) :: lbeg !! Logical flag indicating whether this is the beginning of the half step or not. end subroutine helio_kick_vb_tp + module subroutine helio_setup_initialize_system(self, param) + use swiftest_classes, only : swiftest_parameters + implicit none + class(helio_nbody_system), intent(inout) :: self !! Helio nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + end subroutine helio_setup_initialize_system + module subroutine helio_step_pl(self, system, param, t, dt) use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters implicit none @@ -234,6 +212,7 @@ module subroutine helio_step_tp(self, system, param, t, dt) real(DP), intent(in) :: t !! Current simulation time real(DP), intent(in) :: dt !! Stepsizee end subroutine helio_step_tp + end interface end module helio_classes diff --git a/src/modules/rmvs_classes.f90 b/src/modules/rmvs_classes.f90 index 6ffb7ba1b..0b837ec0a 100644 --- a/src/modules/rmvs_classes.f90 +++ b/src/modules/rmvs_classes.f90 @@ -125,6 +125,14 @@ module function rmvs_encounter_check_tp(self, system, dt) result(lencounter) logical :: lencounter !! Returns true if there is at least one close encounter end function rmvs_encounter_check_tp + module subroutine rmvs_io_write_encounter(t, id1, id2, Gmass1, Gmass2, radius1, radius2, xh1, xh2, vh1, vh2, enc_out) + implicit none + integer(I4B), intent(in) :: id1, id2 + real(DP), intent(in) :: t, Gmass1, Gmass2, radius1, radius2 + real(DP), dimension(:), intent(in) :: xh1, xh2, vh1, vh2 + character(*), intent(in) :: enc_out + end subroutine rmvs_io_write_encounter + module subroutine rmvs_kick_getacch_tp(self, system, param, t, lbeg) use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters implicit none diff --git a/src/modules/swiftest.f90 b/src/modules/swiftest.f90 index 61d45163c..d3f8996f0 100644 --- a/src/modules/swiftest.f90 +++ b/src/modules/swiftest.f90 @@ -10,7 +10,9 @@ module swiftest use rmvs_classes use helio_classes use symba_classes + use fraggle_classes use lambda_function + use walltime_classes !use advisor_annotate !$ use omp_lib implicit none diff --git a/src/modules/swiftest_classes.f90 b/src/modules/swiftest_classes.f90 index 2e4bff8a2..82d684f1a 100644 --- a/src/modules/swiftest_classes.f90 +++ b/src/modules/swiftest_classes.f90 @@ -7,6 +7,81 @@ module swiftest_classes implicit none public + type :: netcdf_parameters + integer(I4B) :: out_type !! NetCDF output type (will be assigned either NF90_DOUBLE or NF90_FLOAT, depending on the user parameter) + integer(I4B) :: ncid !! NetCDF ID for the output file + integer(I4B) :: dimids(3) !! Dimensions of the NetCDF file + integer(I4B) :: time_dimid !! NetCDF ID for the time dimension + integer(I4B) :: id_dimid !! NetCDF ID for the particle id dimension + integer(I4B) :: str_dimid !! NetCDF ID for the character string dimension + integer(I4B) :: time_varid !! NetCDF ID for the time variable + integer(I4B) :: id_varid !! NetCDF ID for the particle name variable + integer(I4B) :: name_varid !! NetCDF ID for the namevariable + integer(I4B) :: ptype_varid !! NetCDF ID for the particle type variable + integer(I4B) :: npl_varid !! NetCDF ID for the number of active massive bodies variable + integer(I4B) :: ntp_varid !! NetCDF ID for the number of active test particles variable + integer(I4B) :: a_varid !! NetCDF ID for the semimajor axis variable + integer(I4B) :: e_varid !! NetCDF ID for the eccentricity variable + integer(I4B) :: inc_varid !! NetCDF ID for the inclination variable + integer(I4B) :: capom_varid !! NetCDF ID for the long. asc. node variable + integer(I4B) :: omega_varid !! NetCDF ID for the arg. periapsis variable + integer(I4B) :: capm_varid !! NetCDF ID for the mean anomaly variable + integer(I4B) :: xhx_varid !! NetCDF ID for the heliocentric position x variable + integer(I4B) :: xhy_varid !! NetCDF ID for the heliocentric position y variable + integer(I4B) :: xhz_varid !! NetCDF ID for the heliocentric position z variable + integer(I4B) :: vhx_varid !! NetCDF ID for the heliocentric velocity x variable + integer(I4B) :: vhy_varid !! NetCDF ID for the heliocentric velocity y variable + integer(I4B) :: vhz_varid !! NetCDF ID for the heliocentric velocity z variable + integer(I4B) :: Gmass_varid !! NetCDF ID for the mass variable + integer(I4B) :: rhill_varid !! NetCDF ID for the hill radius variable + integer(I4B) :: radius_varid !! NetCDF ID for the radius variable + integer(I4B) :: Ip1_varid !! NetCDF ID for the axis 1 principal moment of inertia variable + integer(I4B) :: Ip2_varid !! NetCDF ID for the axis 2 principal moment of inertia variable + integer(I4B) :: Ip3_varid !! NetCDF ID for the axis 3 principal moment of inertia variable + integer(I4B) :: rotx_varid !! NetCDF ID for the rotation x variable + integer(I4B) :: roty_varid !! NetCDF ID for the rotation y variable + integer(I4B) :: rotz_varid !! NetCDF ID for the rotation z variable + integer(I4B) :: k2_varid !! NetCDF ID for the Love number variable + integer(I4B) :: Q_varid !! NetCDF ID for the energy dissipation variable + integer(I4B) :: KE_orb_varid !! NetCDF ID for the system orbital kinetic energy variable + integer(I4B) :: KE_spin_varid !! NetCDF ID for the system spin kinetic energy variable + integer(I4B) :: PE_varid !! NetCDF ID for the system potential energy variable + integer(I4B) :: L_orbx_varid !! NetCDF ID for the system orbital angular momentum x variable + integer(I4B) :: L_orby_varid !! NetCDF ID for the system orbital angular momentum y variable + integer(I4B) :: L_orbz_varid !! NetCDF ID for the system orbital angular momentum z variable + integer(I4B) :: L_spinx_varid !! NetCDF ID for the system spin angular momentum x variable + integer(I4B) :: L_spiny_varid !! NetCDF ID for the system spin angular momentum y variable + integer(I4B) :: L_spinz_varid !! NetCDF ID for the system spin angular momentum z variable + integer(I4B) :: L_escapex_varid !! NetCDF ID for the escaped angular momentum x variable + integer(I4B) :: L_escapey_varid !! NetCDF ID for the escaped angular momentum x variable + integer(I4B) :: L_escapez_varid !! NetCDF ID for the escaped angular momentum x variable + integer(I4B) :: Ecollisions_varid !! NetCDF ID for the energy lost in collisions variable + integer(I4B) :: Euntracked_varid !! NetCDF ID for the energy that is untracked due to loss (untracked potential energy due to mergers and body energy for escaped bodies) + integer(I4B) :: GMescape_varid !! NetCDF ID for the G*Mass of bodies that escape the system + integer(I4B) :: status_varid !! NetCDF ID for the status variable + integer(I4B) :: origin_type_varid !! NetCDF ID for the origin type + integer(I4B) :: origin_time_varid !! NetCDF ID for the origin time + integer(I4B) :: origin_xhx_varid !! NetCDF ID for the origin xh x component + integer(I4B) :: origin_xhy_varid !! NetCDF ID for the origin xh y component + integer(I4B) :: origin_xhz_varid !! NetCDF ID for the origin xh z component + integer(I4B) :: origin_vhx_varid !! NetCDF ID for the origin xh x component + integer(I4B) :: origin_vhy_varid !! NetCDF ID for the origin xh y component + integer(I4B) :: origin_vhz_varid !! NetCDF ID for the origin xh z component + integer(I4B) :: discard_time_varid !! NetCDF ID for the time of discard variable + integer(I4B) :: discard_xhx_varid !! NetCDF ID for the heliocentric position of the body at the time of discard x variable + integer(I4B) :: discard_xhy_varid !! NetCDF ID for the heliocentric position of the body at the time of discard y variable + integer(I4B) :: discard_xhz_varid !! NetCDF ID for the heliocentric position of the body at the time of discard z variable + integer(I4B) :: discard_vhx_varid !! NetCDF ID for the heliocentric velocity of the body at the time of discard x variable + integer(I4B) :: discard_vhy_varid !! NetCDF ID for the heliocentric velocity of the body at the time of discard y variable + integer(I4B) :: discard_vhz_varid !! NetCDF ID for the heliocentric velocity of the body at the time of discard z variable + integer(I4B) :: discard_body_id_varid !! NetCDF ID for the id of the other body involved in the discard + + contains + procedure :: close => netcdf_close !! Closes an open NetCDF file + procedure :: initialize => netcdf_initialize_output !! Initialize a set of parameters used to identify a NetCDF output object + procedure :: open => netcdf_open !! Opens a NetCDF file + end type netcdf_parameters + !******************************************************************************************************************************** ! swiftest_parameters class definitions !******************************************************************************************************************************** @@ -15,21 +90,23 @@ module swiftest_classes !> Each paramter is initialized to a default values. type :: swiftest_parameters integer(I4B) :: integrator = UNKNOWN_INTEGRATOR !! Symbolic name of the nbody integrator used - integer(I4B) :: nplmax = -1 !! Maximum allowed number of massive bodies - integer(I4B) :: ntpmax = -1 !! Maximum allowed number of test particles + integer(I4B) :: maxid = -1 !! The current maximum particle id number real(DP) :: t0 = -1.0_DP !! Integration start time real(DP) :: t = -1.0_DP !! Integration current time real(DP) :: tstop = -1.0_DP !! Integration stop time real(DP) :: dt = -1.0_DP !! Time step + integer(I8B) :: ioutput = 0_I8B !! Output counter character(STRMAX) :: incbfile = CB_INFILE !! Name of input file for the central body character(STRMAX) :: inplfile = PL_INFILE !! Name of input file for massive bodies character(STRMAX) :: intpfile = TP_INFILE !! Name of input file for test particles - character(STRMAX) :: in_type = ASCII_TYPE !! Format of input data files + character(STRMAX) :: in_type = ASCII_TYPE !! Data representation type of input data files + character(STRMAX) :: in_form = XV !! Format of input data files (EL or XV) integer(I4B) :: istep_out = -1 !! Number of time steps between binary outputs - character(STRMAX) :: outfile = BIN_OUTFILE !! Name of output binary file - character(STRMAX) :: out_type = REAL8_TYPE !! Binary format of output file - character(STRMAX) :: out_form = XV !! Data to write to output file + character(STRMAX) :: outfile = NETCDF_OUTFILE !! Name of output binary file + character(STRMAX) :: out_type = NETCDF_DOUBLE_TYPE !! Binary format of output file + character(STRMAX) :: out_form = XVEL !! Data to write to output file character(STRMAX) :: out_stat = 'NEW' !! Open status for output binary file + character(STRMAX) :: particle_out = PARTICLE_OUTFILE !! Name of output particle information file integer(I4B) :: istep_dump = -1 !! Number of time steps between dumps real(DP) :: rmin = -1.0_DP !! Minimum heliocentric radius for test particle real(DP) :: rmax = -1.0_DP !! Maximum heliocentric radius for test particle @@ -59,14 +136,12 @@ module swiftest_classes ! Initial values to pass to the energy report subroutine (usually only used in the case of a restart, otherwise these will be updated with initial conditions values) real(DP) :: Eorbit_orig = 0.0_DP !! Initial orbital energy - real(DP) :: Mtot_orig = 0.0_DP !! Initial system mass - real(DP) :: Lmag_orig = 0.0_DP !! Initial total angular momentum magnitude + real(DP) :: GMtot_orig = 0.0_DP !! Initial system mass real(DP), dimension(NDIM) :: Ltot_orig = 0.0_DP !! Initial total angular momentum vector real(DP), dimension(NDIM) :: Lorbit_orig = 0.0_DP !! Initial orbital angular momentum real(DP), dimension(NDIM) :: Lspin_orig = 0.0_DP !! Initial spin angular momentum vector - real(DP), dimension(NDIM) :: Ltot = 0.0_DP !! System angular momentum vector real(DP), dimension(NDIM) :: Lescape = 0.0_DP !! Angular momentum of bodies that escaped the system (used for bookeeping) - real(DP) :: Mescape = 0.0_DP !! Mass of bodies that escaped the system (used for bookeeping) + real(DP) :: GMescape = 0.0_DP !! Mass of bodies that escaped the system (used for bookeeping) real(DP) :: Ecollisions = 0.0_DP !! Energy lost from system due to collisions real(DP) :: Euntracked = 0.0_DP !! Energy gained from system due to escaped bodies logical :: lfirstenergy = .true. !! This is the first time computing energe @@ -77,25 +152,53 @@ module swiftest_classes logical :: lgr = .false. !! Turn on GR logical :: lyarkovsky = .false. !! Turn on Yarkovsky effect logical :: lyorp = .false. !! Turn on YORP effect + + type(netcdf_parameters) :: nciu !! Object containing NetCDF parameters contains - procedure :: reader => io_param_reader - procedure :: writer => io_param_writer - procedure :: dump => io_dump_param - procedure :: read_from_file => io_read_param_in + procedure :: reader => io_param_reader + procedure :: writer => io_param_writer + procedure :: dump => io_dump_param + procedure :: read_in => io_read_in_param end type swiftest_parameters + + !******************************************************************************************************************************** + ! swiftest_swiftest_particle_info class definitions and method interfaces + !******************************************************************************************************************************* + !> Class definition for the particle origin information object. This object is used to track time, location, and collisional regime + !> of fragments produced in collisional events. + type :: swiftest_particle_info + character(len=NAMELEN) :: name !! Non-unique name + character(len=NAMELEN) :: particle_type !! String containing a description of the particle type (e.g. Central Body, Massive Body, Test Particle) + character(len=NAMELEN) :: origin_type !! String containing a description of the origin of the particle (e.g. Initial Conditions, Supercatastrophic, Disruption, etc.) + real(DP) :: origin_time !! The time of the particle's formation + real(DP), dimension(NDIM) :: origin_xh !! The heliocentric distance vector at the time of the particle's formation + real(DP), dimension(NDIM) :: origin_vh !! The heliocentric velocity vector at the time of the particle's formation + real(DP) :: discard_time !! The time of the particle's discard + character(len=NAMELEN) :: status !! Particle status description: Active, Merged, Fragmented, etc. + real(DP), dimension(NDIM) :: discard_xh !! The heliocentric distance vector at the time of the particle's discard + real(DP), dimension(NDIM) :: discard_vh !! The heliocentric velocity vector at the time of the particle's discard + integer(I4B) :: discard_body_id !! The id of the other body involved in the discard (0 if no other body involved) + contains + procedure :: dump => io_dump_particle_info !! Dumps contents of particle information to file + procedure :: read_in => io_read_in_particle_info !! Read in a particle information object from an open file + procedure :: copy => util_copy_particle_info !! Copies one set of information object components into another, component-by-component + procedure :: set_value => util_set_particle_info !! Sets one or more values of the particle information metadata object + end type swiftest_particle_info + !******************************************************************************************************************************** ! swiftest_base class definitions and methods !******************************************************************************************************************************** type, abstract :: swiftest_base - !! An superclass for a generic Swiftest object - logical :: lintegrate = .false. !! Flag indicating that this object should be integrated in the current step + !! An abstract superclass for a generic Swiftest object contains !! The minimal methods that all systems must have - procedure :: dump => io_dump_swiftest - procedure(abstract_initialize), deferred :: initialize - procedure(abstract_read_frame), deferred :: read_frame - procedure(abstract_write_frame), deferred :: write_frame + procedure :: dump => io_dump_base !! Dump contents to file + procedure :: dump_particle_info => io_dump_particle_info_base !! Dump contents of particle information metadata to file + procedure :: write_frame_netcdf => netcdf_write_frame_base !! I/O routine for writing out a single frame of time-series data for all bodies in the system in NetCDF format + procedure :: write_particle_info_netcdf => netcdf_write_particle_info_base !! Writes out the particle information metadata to NetCDF file + generic :: write_frame => write_frame_netcdf !! Set up generic procedure that will switch between NetCDF or Fortran binary depending on arguments + generic :: write_particle_info => write_particle_info_netcdf end type swiftest_base !******************************************************************************************************************************** @@ -103,34 +206,35 @@ module swiftest_classes !******************************************************************************************************************************** !> A concrete lass for the central body in a Swiftest simulation type, abstract, extends(swiftest_base) :: swiftest_cb - character(len=STRMAX) :: name !! Non-unique name - integer(I4B) :: id = 0 !! External identifier (unique) - real(DP) :: mass = 0.0_DP !! Central body mass (units MU) - real(DP) :: Gmass = 0.0_DP !! Central mass gravitational term G * mass (units GU * MU) - real(DP) :: radius = 0.0_DP !! Central body radius (units DU) - real(DP) :: density = 1.0_DP !! Central body mass density - calculated internally (units MU / DU**3) - real(DP) :: j2rp2 = 0.0_DP !! J2*R^2 term for central body - real(DP) :: j4rp4 = 0.0_DP !! J4*R^2 term for central body - real(DP), dimension(NDIM) :: aobl = 0.0_DP !! Barycentric acceleration due to central body oblatenes - real(DP), dimension(NDIM) :: atide = 0.0_DP !! Barycentric acceleration due to central body oblatenes - real(DP), dimension(NDIM) :: aoblbeg = 0.0_DP !! Barycentric acceleration due to central body oblatenes at beginning of step - real(DP), dimension(NDIM) :: aoblend = 0.0_DP !! Barycentric acceleration due to central body oblatenes at end of step - real(DP), dimension(NDIM) :: atidebeg = 0.0_DP !! Barycentric acceleration due to central body oblatenes at beginning of step - real(DP), dimension(NDIM) :: atideend = 0.0_DP !! Barycentric acceleration due to central body oblatenes at end of step - real(DP), dimension(NDIM) :: xb = 0.0_DP !! Barycentric position (units DU) - real(DP), dimension(NDIM) :: vb = 0.0_DP !! Barycentric velocity (units DU / TU) - real(DP), dimension(NDIM) :: agr = 0.0_DP !! Acceleration due to post-Newtonian correction - real(DP), dimension(NDIM) :: Ip = 0.0_DP !! Unitless principal moments of inertia (I1, I2, I3) / (MR**2). Principal axis rotation assumed. - real(DP), dimension(NDIM) :: rot = 0.0_DP !! Body rotation vector in inertial coordinate frame (units rad / TU) - real(DP) :: k2 = 0.0_DP !! Tidal Love number - real(DP) :: Q = 0.0_DP !! Tidal quality factor - real(DP) :: tlag = 0.0_DP !! Tidal phase lag angle - real(DP), dimension(NDIM) :: L0 = 0.0_DP !! Initial angular momentum of the central body - real(DP), dimension(NDIM) :: dL = 0.0_DP !! Change in angular momentum of the central body + type(swiftest_particle_info) :: info !! Particle metadata information + integer(I4B) :: id = 0 !! External identifier (unique) + real(DP) :: mass = 0.0_DP !! Central body mass (units MU) + real(DP) :: Gmass = 0.0_DP !! Central mass gravitational term G * mass (units GU * MU) + real(DP) :: radius = 0.0_DP !! Central body radius (units DU) + real(DP) :: density = 1.0_DP !! Central body mass density - calculated internally (units MU / DU**3) + real(DP) :: j2rp2 = 0.0_DP !! J2*R^2 term for central body + real(DP) :: j4rp4 = 0.0_DP !! J4*R^2 term for central body + real(DP), dimension(NDIM) :: aobl = 0.0_DP !! Barycentric acceleration due to central body oblatenes + real(DP), dimension(NDIM) :: atide = 0.0_DP !! Barycentric acceleration due to central body oblatenes + real(DP), dimension(NDIM) :: aoblbeg = 0.0_DP !! Barycentric acceleration due to central body oblatenes at beginning of step + real(DP), dimension(NDIM) :: aoblend = 0.0_DP !! Barycentric acceleration due to central body oblatenes at end of step + real(DP), dimension(NDIM) :: atidebeg = 0.0_DP !! Barycentric acceleration due to central body oblatenes at beginning of step + real(DP), dimension(NDIM) :: atideend = 0.0_DP !! Barycentric acceleration due to central body oblatenes at end of step + real(DP), dimension(NDIM) :: xb = 0.0_DP !! Barycentric position (units DU) + real(DP), dimension(NDIM) :: vb = 0.0_DP !! Barycentric velocity (units DU / TU) + real(DP), dimension(NDIM) :: agr = 0.0_DP !! Acceleration due to post-Newtonian correction + real(DP), dimension(NDIM) :: Ip = 0.0_DP !! Unitless principal moments of inertia (I1, I2, I3) / (MR**2). Principal axis rotation assumed. + real(DP), dimension(NDIM) :: rot = 0.0_DP !! Body rotation vector in inertial coordinate frame (units rad / TU) + real(DP) :: k2 = 0.0_DP !! Tidal Love number + real(DP) :: Q = 0.0_DP !! Tidal quality factor + real(DP) :: tlag = 0.0_DP !! Tidal phase lag angle + real(DP), dimension(NDIM) :: L0 = 0.0_DP !! Initial angular momentum of the central body + real(DP), dimension(NDIM) :: dL = 0.0_DP !! Change in angular momentum of the central body contains - procedure :: initialize => io_read_cb_in !! I/O routine for reading in central body data - procedure :: read_frame => io_read_frame_cb !! I/O routine for reading out a single frame of time-series data for the central body - procedure :: write_frame => io_write_frame_cb !! I/O routine for writing out a single frame of time-series data for the central body + procedure :: read_in => io_read_in_cb !! I/O routine for reading in central body data + procedure :: read_frame => io_read_frame_cb !! I/O routine for reading out a single frame of time-series data for the central body + procedure :: write_frame_bin => io_write_frame_cb !! I/O routine for writing out a single frame of time-series data for the central body + generic :: write_frame => write_frame_bin !! Write a frame (either binary or NetCDF, using generic procedures) end type swiftest_cb !******************************************************************************************************************************** @@ -139,29 +243,29 @@ module swiftest_classes !> An abstract class for a generic collection of Swiftest bodies type, abstract, extends(swiftest_base) :: swiftest_body !! Superclass that defines the generic elements of a Swiftest particle - logical :: lfirst = .true. !! Run the current step as a first - integer(I4B) :: nbody = 0 !! Number of bodies - character(len=STRMAX), dimension(:), allocatable :: name !! Non-unique name - integer(I4B), dimension(:), allocatable :: id !! External identifier (unique) - integer(I4B), dimension(:), allocatable :: status !! An integrator-specific status indicator - logical, dimension(:), allocatable :: ldiscard !! Body should be discarded - logical, dimension(:), allocatable :: lmask !! Logical mask used to select a subset of bodies when performing certain operations (drift, kick, accel, etc.) - real(DP), dimension(:), allocatable :: mu !! G * (Mcb + [m]) - real(DP), dimension(:,:), allocatable :: xh !! Heliocentric position - real(DP), dimension(:,:), allocatable :: vh !! Heliocentric velocity - real(DP), dimension(:,:), allocatable :: xb !! Barycentric position - real(DP), dimension(:,:), allocatable :: vb !! Barycentric velocity - real(DP), dimension(:,:), allocatable :: ah !! Total heliocentric acceleration - real(DP), dimension(:,:), allocatable :: aobl !! Barycentric accelerations of bodies due to central body oblatenes - real(DP), dimension(:,:), allocatable :: atide !! Tanngential component of acceleration of bodies due to tides - real(DP), dimension(:,:), allocatable :: agr !! Acceleration due to post-Newtonian correction - real(DP), dimension(:), allocatable :: ir3h !! Inverse heliocentric radius term (1/rh**3) - real(DP), dimension(:), allocatable :: a !! Semimajor axis (pericentric distance for a parabolic orbit) - real(DP), dimension(:), allocatable :: e !! Eccentricity - real(DP), dimension(:), allocatable :: inc !! Inclination - real(DP), dimension(:), allocatable :: capom !! Longitude of ascending node - real(DP), dimension(:), allocatable :: omega !! Argument of pericenter - real(DP), dimension(:), allocatable :: capm !! Mean anomaly + logical :: lfirst = .true. !! Run the current step as a first + integer(I4B) :: nbody = 0 !! Number of bodies + type(swiftest_particle_info), dimension(:), allocatable :: info !! Particle metadata information + integer(I4B), dimension(:), allocatable :: id !! External identifier (unique) + integer(I4B), dimension(:), allocatable :: status !! An integrator-specific status indicator + logical, dimension(:), allocatable :: ldiscard !! Body should be discarded + logical, dimension(:), allocatable :: lmask !! Logical mask used to select a subset of bodies when performing certain operations (drift, kick, accel, etc.) + real(DP), dimension(:), allocatable :: mu !! G * (Mcb + [m]) + real(DP), dimension(:,:), allocatable :: xh !! Swiftestcentric position + real(DP), dimension(:,:), allocatable :: vh !! Swiftestcentric velocity + real(DP), dimension(:,:), allocatable :: xb !! Barycentric position + real(DP), dimension(:,:), allocatable :: vb !! Barycentric velocity + real(DP), dimension(:,:), allocatable :: ah !! Total heliocentric acceleration + real(DP), dimension(:,:), allocatable :: aobl !! Barycentric accelerations of bodies due to central body oblatenes + real(DP), dimension(:,:), allocatable :: atide !! Tanngential component of acceleration of bodies due to tides + real(DP), dimension(:,:), allocatable :: agr !! Acceleration due to post-Newtonian correction + real(DP), dimension(:), allocatable :: ir3h !! Inverse heliocentric radius term (1/rh**3) + real(DP), dimension(:), allocatable :: a !! Semimajor axis (pericentric distance for a parabolic orbit) + real(DP), dimension(:), allocatable :: e !! Eccentricity + real(DP), dimension(:), allocatable :: inc !! Inclination + real(DP), dimension(:), allocatable :: capom !! Longitude of ascending node + real(DP), dimension(:), allocatable :: omega !! Argument of pericenter + real(DP), dimension(:), allocatable :: capm !! Mean anomaly !! Note to developers: If you add components to this class, be sure to update methods and subroutines that traverse the !! component list, such as setup_body and util_spill contains @@ -171,24 +275,25 @@ module swiftest_classes procedure(abstract_step_body), deferred :: step procedure(abstract_accel), deferred :: accel ! These are concrete because the implementation is the same for all types of particles - procedure :: drift => drift_body !! Loop through bodies and call Danby drift routine on heliocentric variables - procedure :: v2pv => gr_vh2pv_body !! Converts from velocity to psudeovelocity for GR calculations using symplectic integrators - procedure :: pv2v => gr_pv2vh_body !! Converts from psudeovelocity to velocity for GR calculations using symplectic integrators - procedure :: initialize => io_read_body_in !! Read in body initial conditions from a file - procedure :: read_frame => io_read_frame_body !! I/O routine for writing out a single frame of time-series data for the central body - procedure :: write_frame => io_write_frame_body !! I/O routine for writing out a single frame of time-series data for the central body - procedure :: accel_obl => obl_acc_body !! Compute the barycentric accelerations of bodies due to the oblateness of the central body - procedure :: el2xv => orbel_el2xv_vec !! Convert orbital elements to position and velocity vectors - procedure :: xv2el => orbel_xv2el_vec !! Convert position and velocity vectors to orbital elements - procedure :: setup => setup_body !! A constructor that sets the number of bodies and allocates all allocatable arrays - procedure :: accel_user => user_kick_getacch_body !! Add user-supplied heliocentric accelerations to planets - procedure :: append => util_append_body !! Appends elements from one structure to another - procedure :: fill => util_fill_body !! "Fills" bodies from one object into another depending on the results of a mask (uses the UNPACK intrinsic) - procedure :: resize => util_resize_body !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. - procedure :: set_ir3 => util_set_ir3h !! Sets the inverse heliocentric radius term (1/rh**3) - procedure :: sort => util_sort_body !! Sorts body arrays by a sortable componen - procedure :: rearrange => util_sort_rearrange_body !! Rearranges the order of array elements of body based on an input index array. Used in sorting methods - procedure :: spill => util_spill_body !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) + procedure :: drift => drift_body !! Loop through bodies and call Danby drift routine on heliocentric variables + procedure :: v2pv => gr_vh2pv_body !! Converts from velocity to psudeovelocity for GR calculations using symplectic integrators + procedure :: pv2v => gr_pv2vh_body !! Converts from psudeovelocity to velocity for GR calculations using symplectic integrators + procedure :: read_in => io_read_in_body !! Read in body initial conditions from a file + procedure :: read_frame => io_read_frame_body !! I/O routine for writing out a single frame of time-series data for the central body + procedure :: write_frame_bin => io_write_frame_body !! I/O routine for writing out a single frame of time-series data for the central body + procedure :: accel_obl => obl_acc_body !! Compute the barycentric accelerations of bodies due to the oblateness of the central body + procedure :: el2xv => orbel_el2xv_vec !! Convert orbital elements to position and velocity vectors + procedure :: xv2el => orbel_xv2el_vec !! Convert position and velocity vectors to orbital elements + procedure :: setup => setup_body !! A constructor that sets the number of bodies and allocates all allocatable arrays + procedure :: accel_user => user_kick_getacch_body !! Add user-supplied heliocentric accelerations to planets + procedure :: append => util_append_body !! Appends elements from one structure to another + procedure :: fill => util_fill_body !! "Fills" bodies from one object into another depending on the results of a mask (uses the UNPACK intrinsic) + procedure :: resize => util_resize_body !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. + procedure :: set_ir3 => util_set_ir3h !! Sets the inverse heliocentric radius term (1/rh**3) + procedure :: sort => util_sort_body !! Sorts body arrays by a sortable componen + procedure :: rearrange => util_sort_rearrange_body !! Rearranges the order of array elements of body based on an input index array. Used in sorting methods + procedure :: spill => util_spill_body !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) + generic :: write_frame => write_frame_bin !! Add the generic write frame for Fortran binary files end type swiftest_body !******************************************************************************************************************************** @@ -218,7 +323,7 @@ module swiftest_classes ! Massive body-specific concrete methods ! These are concrete because they are the same implemenation for all integrators procedure :: discard => discard_pl !! Placeholder method for discarding massive bodies - procedure :: eucl_index => eucl_dist_index_plpl !! Sets up the (i, j) -> k indexing used for the single-loop blocking Euclidean distance matrix + procedure :: index => util_index_eucl_plpl !! Sets up the (i, j) -> k indexing used for the single-loop blocking Euclidean distance matrix procedure :: accel_int => kick_getacch_int_pl !! Compute direct cross (third) term heliocentric accelerations of massive bodies procedure :: accel_obl => obl_acc_pl !! Compute the barycentric accelerations of bodies due to the oblateness of the central body procedure :: setup => setup_pl !! A base constructor that sets the number of bodies and allocates and initializes all arrays @@ -226,6 +331,9 @@ module swiftest_classes procedure :: append => util_append_pl !! Appends elements from one structure to another procedure :: h2b => util_coord_h2b_pl !! Convert massive bodies from heliocentric to barycentric coordinates (position and velocity) procedure :: b2h => util_coord_b2h_pl !! Convert massive bodies from barycentric to heliocentric coordinates (position and velocity) + procedure :: vh2vb => util_coord_vh2vb_pl !! Convert massive bodies from heliocentric to barycentric coordinates (velocity only) + procedure :: vb2vh => util_coord_vb2vh_pl !! Convert massive bodies from barycentric to heliocentric coordinates (velocity only) + procedure :: xh2xb => util_coord_xh2xb_pl !! Convert massive bodies from heliocentric to barycentric coordinates (position only) procedure :: fill => util_fill_pl !! "Fills" bodies from one object into another depending on the results of a mask (uses the UNPACK intrinsic) procedure :: resize => util_resize_pl !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. procedure :: set_beg_end => util_set_beg_end_pl !! Sets the beginning and ending positions and velocities of planets. @@ -242,9 +350,11 @@ module swiftest_classes !> An abstract class for a generic collection of Swiftest test particles type, abstract, extends(swiftest_body) :: swiftest_tp !! Superclass that defines the generic elements of a Swiftest test particle - integer(I4B), dimension(:), allocatable :: isperi !! Perihelion passage flag - real(DP), dimension(:), allocatable :: peri !! Perihelion distance - real(DP), dimension(:), allocatable :: atp !! Semimajor axis following perihelion passage + integer(I4B), dimension(:), allocatable :: isperi !! Perihelion passage flag + real(DP), dimension(:), allocatable :: peri !! Perihelion distance + real(DP), dimension(:), allocatable :: atp !! Semimajor axis following perihelion passage + integer(I4B), dimension(:,:), allocatable :: k_pltp !! Index array used to convert flattened the body-body comparison upper triangular matrix + integer(I8B) :: npltp !! Number of pl-tp comparisons in the flattened upper triangular matrix !! Note to developers: If you add components to this class, be sure to update methods and subroutines that traverse the !! component list, such as setup_tp and util_spill_tp contains @@ -257,6 +367,9 @@ module swiftest_classes procedure :: append => util_append_tp !! Appends elements from one structure to another procedure :: h2b => util_coord_h2b_tp !! Convert test particles from heliocentric to barycentric coordinates (position and velocity) procedure :: b2h => util_coord_b2h_tp !! Convert test particles from barycentric to heliocentric coordinates (position and velocity) + procedure :: vb2vh => util_coord_vb2vh_tp !! Convert test particles from barycentric to heliocentric coordinates (velocity only) + procedure :: vh2vb => util_coord_vh2vb_tp !! Convert test particles from heliocentric to barycentric coordinates (velocity only) + procedure :: xh2xb => util_coord_xh2xb_tp !! Convert test particles from heliocentric to barycentric coordinates (position only) procedure :: fill => util_fill_tp !! "Fills" bodies from one object into another depending on the results of a mask (uses the UNPACK intrinsic) procedure :: get_peri => util_peri_tp !! Determine system pericenter passages for test particles procedure :: resize => util_resize_tp !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. @@ -270,62 +383,72 @@ module swiftest_classes ! swiftest_nbody_system class definitions and methods !******************************************************************************************************************************** !> An abstract class for a basic Swiftest nbody system - type, abstract, extends(swiftest_base) :: swiftest_nbody_system + type, abstract :: swiftest_nbody_system !! This superclass contains a minimial system of a set of test particles (tp), massive bodies (pl), and a central body (cb) - class(swiftest_cb), allocatable :: cb !! Central body data structure - class(swiftest_pl), allocatable :: pl !! Massive body data structure - class(swiftest_tp), allocatable :: tp !! Test particle data structure - class(swiftest_tp), allocatable :: tp_discards !! Discarded test particle data structure - class(swiftest_pl), allocatable :: pl_discards !! Discarded massive body particle data structure - real(DP) :: Gmtot = 0.0_DP !! Total system mass - used for barycentric coordinate conversion - real(DP) :: ke_orbit = 0.0_DP !! System orbital kinetic energy - real(DP) :: ke_spin = 0.0_DP !! System spin kinetic energy - real(DP) :: pe = 0.0_DP !! System potential energy - real(DP) :: te = 0.0_DP !! System total energy - real(DP), dimension(NDIM) :: Lorbit = 0.0_DP !! System orbital angular momentum vector - real(DP), dimension(NDIM) :: Lspin = 0.0_DP !! System spin angular momentum vector - real(DP), dimension(NDIM) :: Lescape = 0.0_DP !! Angular momentum of bodies that escaped the system (used for bookeeping) - real(DP) :: Mescape = 0.0_DP !! Mass of bodies that escaped the system (used for bookeeping) - real(DP) :: Ecollisions = 0.0_DP !! Energy lost from system due to collisions - real(DP) :: Euntracked = 0.0_DP !! Energy gained from system due to escaped bodies - logical :: lbeg !! True if this is the beginning of a step. This is used so that test particle steps can be calculated - !! separately from massive bodies. Massive body variables are saved at half steps, and passed to - !! the test particles - integer(I4B) :: maxid = -1 !! The current maximum particle id number + class(swiftest_cb), allocatable :: cb !! Central body data structure + class(swiftest_pl), allocatable :: pl !! Massive body data structure + class(swiftest_tp), allocatable :: tp !! Test particle data structure + class(swiftest_tp), allocatable :: tp_discards !! Discarded test particle data structure + class(swiftest_pl), allocatable :: pl_discards !! Discarded massive body particle data structure + real(DP) :: GMtot = 0.0_DP !! Total system mass - used for barycentric coordinate conversion + real(DP) :: ke_orbit = 0.0_DP !! System orbital kinetic energy + real(DP) :: ke_spin = 0.0_DP !! System spin kinetic energy + real(DP) :: pe = 0.0_DP !! System potential energy + real(DP) :: te = 0.0_DP !! System total energy + real(DP) :: oblpot = 0.0_DP !! System potential energy due to oblateness of the central body + real(DP), dimension(NDIM) :: Lorbit = 0.0_DP !! System orbital angular momentum vector + real(DP), dimension(NDIM) :: Lspin = 0.0_DP !! System spin angular momentum vector + real(DP), dimension(NDIM) :: Ltot = 0.0_DP !! System angular momentum vector + logical :: lbeg !! True if this is the beginning of a step. This is used so that test particle steps can be calculated + !! separately from massive bodies. Massive body variables are saved at half steps, and passed to + !! the test particles contains !> Each integrator will have its own version of the step procedure(abstract_step_system), deferred :: step ! Concrete classes that are common to the basic integrator (only test particles considered for discard) - procedure :: discard => discard_system !! Perform a discard step on the system - procedure :: conservation_report => io_conservation_report !! Compute energy and momentum and print out the change with time - procedure :: dump => io_dump_system !! Dump the state of the system to a file - procedure :: read_frame => io_read_frame_system !! Read in a frame of input data from file - procedure :: write_discard => io_write_discard !! Write out information about discarded test particles - procedure :: write_frame => io_write_frame_system !! Append a frame of output data to file - procedure :: initialize => setup_initialize_system !! Initialize the system from input files - procedure :: step_spin => tides_step_spin_system !! Steps the spins of the massive & central bodies due to tides. - procedure :: set_msys => util_set_msys !! Sets the value of msys from the masses of system bodies. - procedure :: get_energy_and_momentum => util_get_energy_momentum_system !! Calculates the total system energy and momentum - procedure :: rescale => util_rescale_system !! Rescales the system into a new set of units - procedure :: validate_ids => util_valid_id_system !! Validate the numerical ids passed to the system and save the maximum value + procedure :: discard => discard_system !! Perform a discard step on the system + procedure :: conservation_report => io_conservation_report !! Compute energy and momentum and print out the change with time + procedure :: dump => io_dump_system !! Dump the state of the system to a file + procedure :: get_old_t_final => io_get_old_t_final_system !! Validates the dump file to check whether the dump file initial conditions duplicate the last frame of the binary output. + procedure :: read_frame => io_read_frame_system !! Read in a frame of input data from file + procedure :: read_particle_info => io_read_particle_info_system !! Read in particle metadata from file + procedure :: write_discard => io_write_discard !! Write out information about discarded test particles + procedure :: write_frame => io_write_frame_system !! Append a frame of output data to file + procedure :: write_hdr_bin => io_write_hdr_system !! Write a header for an output frame in Fortran binary format + procedure :: write_hdr_netcdf => netcdf_write_hdr_system !! Write a header for an output frame in NetCDF format + procedure :: obl_pot => obl_pot_system !! Compute the contribution to the total gravitational potential due solely to the oblateness of the central body + procedure :: initialize => setup_initialize_system !! Initialize the system from input files + procedure :: init_particle_info => setup_initialize_particle_info_system !! Initialize the system from input files + procedure :: step_spin => tides_step_spin_system !! Steps the spins of the massive & central bodies due to tides. + procedure :: set_msys => util_set_msys !! Sets the value of msys from the masses of system bodies. + procedure :: get_energy_and_momentum => util_get_energy_momentum_system !! Calculates the total system energy and momentum + procedure :: rescale => util_rescale_system !! Rescales the system into a new set of units + procedure :: validate_ids => util_valid_id_system !! Validate the numerical ids passed to the system and save the maximum value + generic :: write_hdr => write_hdr_bin, write_hdr_netcdf !! Generic method call for writing headers end type swiftest_nbody_system type :: swiftest_encounter integer(I4B) :: nenc !! Total number of encounters logical, dimension(:), allocatable :: lvdotr !! relative vdotr flag integer(I4B), dimension(:), allocatable :: status !! status of the interaction + integer(I8B), dimension(:), allocatable :: kidx !! index value of the encounter from the master k_plpl encounter list integer(I4B), dimension(:), allocatable :: index1 !! position of the first body in the encounter integer(I4B), dimension(:), allocatable :: index2 !! position of the second body in the encounter + integer(I4B), dimension(:), allocatable :: id1 !! id of the first body in the encounter + integer(I4B), dimension(:), allocatable :: id2 !! id of the second body in the encounter real(DP), dimension(:,:), allocatable :: x1 !! the position of body 1 in the encounter real(DP), dimension(:,:), allocatable :: x2 !! the position of body 2 in the encounter real(DP), dimension(:,:), allocatable :: v1 !! the velocity of body 1 in the encounter real(DP), dimension(:,:), allocatable :: v2 !! the velocity of body 2 in the encounter + real(DP), dimension(:), allocatable :: t !! Time of encounter contains procedure :: setup => setup_encounter !! A constructor that sets the number of encounters and allocates and initializes all arrays + procedure :: append => util_append_encounter !! Appends elements from one structure to another procedure :: copy => util_copy_encounter !! Copies elements from the source encounter list into self. procedure :: spill => util_spill_encounter !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) procedure :: resize => util_resize_encounter !! Checks the current size of the encounter list against the required size and extends it by a factor of 2 more than requested if it is too small. + procedure :: write => io_write_encounter !! Write close encounter data to output binary file end type swiftest_encounter abstract interface @@ -345,12 +468,6 @@ subroutine abstract_accel(self, system, param, t, lbeg) logical, intent(in) :: lbeg !! Optional argument that determines whether or not this is the beginning or end of the step end subroutine abstract_accel - subroutine abstract_initialize(self, param) - import swiftest_base, swiftest_parameters - class(swiftest_base), intent(inout) :: self !! Swiftest base object - class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - end subroutine abstract_initialize - subroutine abstract_kick_body(self, system, param, t, dt, lbeg) import swiftest_body, swiftest_nbody_system, swiftest_parameters, DP implicit none @@ -362,14 +479,13 @@ subroutine abstract_kick_body(self, system, param, t, dt, lbeg) logical, intent(in) :: lbeg !! Logical flag indicating whether this is the beginning of the half step or not. end subroutine abstract_kick_body - subroutine abstract_read_frame(self, iu, param, form, ierr) + function abstract_read_frame(self, iu, param) result(ierr) import DP, I4B, swiftest_base, swiftest_parameters class(swiftest_base), intent(inout) :: self !! Swiftest base object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code - end subroutine abstract_read_frame + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + end function abstract_read_frame subroutine abstract_set_mu(self, cb) import swiftest_body, swiftest_cb @@ -395,13 +511,6 @@ subroutine abstract_step_system(self, param, t, dt) real(DP), intent(in) :: t !! Simulation time real(DP), intent(in) :: dt !! Current stepsize end subroutine abstract_step_system - - subroutine abstract_write_frame(self, iu, param) - import DP, I4B, swiftest_base, swiftest_parameters - class(swiftest_base), intent(in) :: self !! Swiftest base object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - end subroutine abstract_write_frame end interface interface @@ -452,35 +561,18 @@ module pure elemental subroutine drift_one(mu, px, py, pz, vx, vy, vz, dt, iflag integer(I4B), intent(out) :: iflag !! iflag : error status flag for Danby drift (0 = OK, nonzero = ERROR) end subroutine drift_one - module subroutine eucl_dist_index_plpl(self) + module subroutine util_index_eucl_plpl(self, param) implicit none - class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine - module subroutine fragmentation_initialize(system, param, family, x, v, L_spin, Ip, mass, radius, & - nfrag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, Qloss, lfailure) - implicit none - class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - integer(I4B), dimension(:), intent(in) :: family !! Index of bodies involved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Two-body equivalent position, vector, spin momentum, and rotational inertia values for the collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Two-body equivalent mass and radii for the bodies in the collision - integer(I4B), intent(inout) :: nfrag !! Number of fragments to generate - real(DP), dimension(:), allocatable, intent(inout) :: m_frag, rad_frag !! Distribution of fragment mass and radii - real(DP), dimension(:,:), allocatable, intent(inout) :: Ip_frag !! Fragment rotational inertia vectors - real(DP), dimension(:,:), allocatable, intent(inout) :: xb_frag, vb_frag, rot_frag !! Fragment barycentric position, barycentric velocity, and rotation vectors - real(DP), intent(inout) :: Qloss !! Energy lost during the collision - logical, intent(out) :: lfailure !! Answers the question: Should this have been a merger instead? - end subroutine fragmentation_initialize - - module subroutine fragmentation_regime(Mcb, m1, m2, rad1, rad2, xh1, xh2, vb1, vb2, den1, den2, regime, Mlr, Mslr, mtiny, Qloss) - implicit none - integer(I4B), intent(out) :: regime - real(DP), intent(out) :: Mlr, Mslr - real(DP), intent(in) :: Mcb, m1, m2, rad1, rad2, den1, den2, mtiny - real(DP), dimension(:), intent(in) :: xh1, xh2, vb1, vb2 - real(DP), intent(out) :: Qloss !! Energy lost during the collision - end subroutine fragmentation_regime + module subroutine util_index_eucl_pltp(self, pl, param) + implicit none + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine module pure subroutine gr_kick_getaccb_ns_body(self, system, param) implicit none @@ -511,9 +603,9 @@ module pure subroutine gr_pseudovel2vel(param, mu, xh, pv, vh) implicit none class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters real(DP), intent(in) :: mu !! G * (Mcb + m), G = gravitational constant, Mcb = mass of central body, m = mass of body - real(DP), dimension(:), intent(in) :: xh !! Heliocentric position vector + real(DP), dimension(:), intent(in) :: xh !! Swiftestcentric position vector real(DP), dimension(:), intent(in) :: pv !! Pseudovelocity velocity vector - see Saha & Tremain (1994), eq. (32) - real(DP), dimension(:), intent(out) :: vh !! Heliocentric velocity vector + real(DP), dimension(:), intent(out) :: vh !! Swiftestcentric velocity vector end subroutine gr_pseudovel2vel module pure subroutine gr_pv2vh_body(self, param) @@ -526,8 +618,8 @@ module pure subroutine gr_vel2pseudovel(param, mu, xh, vh, pv) implicit none class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters real(DP), intent(in) :: mu !! G * (Mcb + m), G = gravitational constant, Mcb = mass of central body, m = mass of body - real(DP), dimension(:), intent(in) :: xh !! Heliocentric position vector - real(DP), dimension(:), intent(in) :: vh !! Heliocentric velocity vector + real(DP), dimension(:), intent(in) :: xh !! Swiftestcentric position vector + real(DP), dimension(:), intent(in) :: vh !! Swiftestcentric velocity vector real(DP), dimension(:), intent(out) :: pv !! Pseudovelocity vector - see Saha & Tremain (1994), eq. (32) end subroutine gr_vel2pseudovel @@ -550,11 +642,24 @@ module subroutine io_dump_param(self, param_file_name) character(len=*), intent(in) :: param_file_name !! Parameter input file name (i.e. param.in) end subroutine io_dump_param - module subroutine io_dump_swiftest(self, param) + module subroutine io_dump_particle_info_base(self, param, idx) + implicit none + class(swiftest_base), intent(inout) :: self !! Swiftest base object (can be cb, pl, or tp) + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + integer(I4B), dimension(:), optional, intent(in) :: idx !! Array of test particle indices to append to the particle file + end subroutine io_dump_particle_info_base + + module subroutine io_dump_particle_info(self, iu) + implicit none + class(swiftest_particle_info), intent(in) :: self !! Swiftest particle info metadata object + integer(I4B), intent(in) :: iu !! Open unformatted file unit number + end subroutine io_dump_particle_info + + module subroutine io_dump_base(self, param) implicit none class(swiftest_base), intent(inout) :: self !! Swiftest base object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - end subroutine io_dump_swiftest + end subroutine io_dump_base module subroutine io_dump_system(self, param) implicit none @@ -569,6 +674,13 @@ module function io_get_args(integrator, param_file_name) result(ierr) integer(I4B) :: ierr !! I/O error code end function io_get_args + module function io_get_old_t_final_system(self, param) result(old_t_final) + implicit none + class(swiftest_nbody_system), intent(in) :: self + class(swiftest_parameters), intent(in) :: param + real(DP) :: old_t_final + end function io_get_old_t_final_system + module function io_get_token(buffer, ifirst, ilast, ierr) result(token) implicit none character(len=*), intent(in) :: buffer !! Input string buffer @@ -600,55 +712,64 @@ module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg) character(len=*), intent(inout) :: iomsg !! Message to pass if iostat /= 0 end subroutine io_param_writer - module subroutine io_read_body_in(self, param) + module subroutine io_read_in_body(self, param) implicit none class(swiftest_body), intent(inout) :: self !! Swiftest body object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - end subroutine io_read_body_in + end subroutine io_read_in_body - module subroutine io_read_cb_in(self, param) + module subroutine io_read_in_cb(self, param) implicit none class(swiftest_cb), intent(inout) :: self !! Swiftest central body object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - end subroutine io_read_cb_in + end subroutine io_read_in_cb - module subroutine io_read_param_in(self, param_file_name) + module subroutine io_read_in_param(self, param_file_name) implicit none class(swiftest_parameters), intent(inout) :: self !! Current run configuration parameters character(len=*), intent(in) :: param_file_name !! Parameter input file name (i.e. param.in) - end subroutine io_read_param_in + end subroutine io_read_in_param - module subroutine io_read_frame_body(self, iu, param, form, ierr) + module subroutine io_read_in_particle_info(self, iu) implicit none - class(swiftest_body), intent(inout) :: self !! Swiftest body object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to - class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code - end subroutine io_read_frame_body + class(swiftest_particle_info), intent(inout) :: self !! Particle metadata information object + integer(I4B), intent(in) :: iu !! Open file unit number + end subroutine io_read_in_particle_info - module subroutine io_read_frame_cb(self, iu, param, form, ierr) + module function io_read_frame_body(self, iu, param) result(ierr) implicit none - class(swiftest_cb), intent(inout) :: self !! Swiftest central body object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to - class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code - end subroutine io_read_frame_cb + class(swiftest_body), intent(inout) :: self !! Swiftest body object + integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + end function io_read_frame_body + + module function io_read_frame_cb(self, iu, param) result(ierr) + implicit none + class(swiftest_cb), intent(inout) :: self !! Swiftest central body object + integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + end function io_read_frame_cb - module subroutine io_read_frame_system(self, iu, param, form, ierr) + module function io_read_frame_system(self, iu, param) result(ierr) implicit none class(swiftest_nbody_system),intent(inout) :: self !! Swiftest system object integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - character(*), intent(in) :: form !! Input format code ("XV" or "EL") - integer(I4B), intent(out) :: ierr !! Error code - end subroutine io_read_frame_system + integer(I4B) :: ierr !! Error code: returns 0 if the read is successful + end function io_read_frame_system + + module subroutine io_read_particle_info_system(self, param) + implicit none + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + end subroutine io_read_particle_info_system module subroutine io_write_discard(self, param) implicit none class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters end subroutine io_write_discard module subroutine io_toupper(string) @@ -656,13 +777,12 @@ module subroutine io_toupper(string) character(*), intent(inout) :: string !! String to make upper case end subroutine io_toupper - module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, radius2, & - xh1, xh2, vh1, vh2, enc_out, out_type) + module subroutine io_write_encounter(self, pl, encbody, param) implicit none - integer(I4B), intent(in) :: name1, name2 - real(DP), intent(in) :: t, mass1, mass2, radius1, radius2 - real(DP), dimension(:), intent(in) :: xh1, xh2, vh1, vh2 - character(*), intent(in) :: enc_out, out_type + class(swiftest_encounter), intent(in) :: self !! Swiftest encounter list object + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object + class(swiftest_body), intent(in) :: encbody !! Encountering body - Swiftest generic body object (pl or tp) + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine io_write_encounter module subroutine io_write_frame_body(self, iu, param) @@ -679,16 +799,62 @@ module subroutine io_write_frame_cb(self, iu, param) class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine io_write_frame_cb - module subroutine io_write_frame_system(self, iu, param) + module subroutine io_write_frame_encounter(iu, t, id1, id2, Gmass1, Gmass2, radius1, radius2, xh1, xh2, vh1, vh2) implicit none - class(swiftest_nbody_system), intent(in) :: self !! Swiftest system object - integer(I4B), intent(inout) :: iu !! Unit number for the output file to write frame to - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + integer(I4B), intent(in) :: iu !! Open file unit number + real(DP), intent(in) :: t !! Time of encounter + integer(I4B), intent(in) :: id1, id2 !! ids of the two encountering bodies + real(DP), intent(in) :: Gmass1, Gmass2 !! G*mass of the two encountering bodies + real(DP), intent(in) :: radius1, radius2 !! Radii of the two encountering bodies + real(DP), dimension(:), intent(in) :: xh1, xh2 !! Swiftestcentric position vectors of the two encountering bodies + real(DP), dimension(:), intent(in) :: vh1, vh2 !! Swiftestcentric velocity vectors of the two encountering bodies + end subroutine io_write_frame_encounter + + module subroutine io_write_frame_system(self, param) + implicit none + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters end subroutine io_write_frame_system - module pure subroutine kick_getacch_int_pl(self) + module subroutine io_write_hdr_system(self, iu, param) + implicit none + class(swiftest_nbody_system), intent(in) :: self !! Swiftest nbody system object + integer(I4B), intent(inout) :: iu !! Output file unit number + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine io_write_hdr_system + + module subroutine kick_getacch_int_all_pl(npl, nplpl, k_plpl, x, Gmass, radius, acc) + implicit none + integer(I4B), intent(in) :: npl !! Number of massive bodies + integer(I8B), intent(in) :: nplpl !! Number of massive body interactions to compute + integer(I4B), dimension(:,:), intent(in) :: k_plpl !! Array of interaction pair indices (flattened upper triangular matrix) + real(DP), dimension(:,:), intent(in) :: x !! Position vector array + real(DP), dimension(:), intent(in) :: Gmass !! Array of massive body G*mass + real(DP), dimension(:), intent(in) :: radius !! Array of massive body radii + real(DP), dimension(:,:), intent(inout) :: acc !! Acceleration vector array + end subroutine kick_getacch_int_all_pl + + module pure subroutine kick_getacch_int_one_pl(rji2, xr, yr, zr, Gmi, Gmj, axi, ayi, azi, axj, ayj, azj) + implicit none + real(DP), intent(in) :: rji2 !! Square of distance between the two bodies + real(DP), intent(in) :: xr, yr, zr !! Distances between the two bodies in x, y, and z directions + real(DP), intent(in) :: Gmi !! G*mass of body i + real(DP), intent(in) :: Gmj !! G*mass of body j + real(DP), intent(inout) :: axi, ayi, azi !! Acceleration vector components of body i + real(DP), intent(inout) :: axj, ayj, azj !! Acceleration vector components of body j + end subroutine kick_getacch_int_one_pl + + module pure subroutine kick_getacch_int_one_tp(rji2, xr, yr, zr, Gmpl, ax, ay, az) implicit none - class(swiftest_pl), intent(inout) :: self + real(DP), intent(in) :: rji2 !! Square of distance between the test particle and massive body + real(DP), intent(in) :: xr, yr, zr !! Distances between the two bodies in x, y, and z directions + real(DP), intent(in) :: Gmpl !! G*mass of massive body + real(DP), intent(inout) :: ax, ay, az !! Acceleration vector components of test particle + end subroutine kick_getacch_int_one_tp + + module subroutine kick_getacch_int_pl(self) + implicit none + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object end subroutine kick_getacch_int_pl module pure subroutine kick_getacch_int_tp(self, GMpl, xhp, npl) @@ -699,6 +865,51 @@ module pure subroutine kick_getacch_int_tp(self, GMpl, xhp, npl) integer(I4B), intent(in) :: npl !! Number of active massive bodies end subroutine kick_getacch_int_tp + module subroutine netcdf_close(self, param) + implicit none + class(netcdf_parameters), intent(inout) :: self !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_close + + module subroutine netcdf_initialize_output(self, param) + implicit none + class(netcdf_parameters), intent(inout) :: self !! Parameters used to for writing a NetCDF dataset to file + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_initialize_output + + module subroutine netcdf_open(self, param) + implicit none + class(netcdf_parameters), intent(inout) :: self !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_open + + module subroutine netcdf_write_frame_base(self, iu, param) + implicit none + class(swiftest_base), intent(in) :: self !! Swiftest base object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to for writing a NetCDF dataset to file + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_write_frame_base + + module subroutine netcdf_write_frame_system(self, iu, param) + implicit none + class(swiftest_nbody_system), intent(in) :: self !! Swiftest system object + integer(I4B), intent(inout) :: iu !! Parameters used to for writing a NetCDF dataset to file + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_write_frame_system + + module subroutine netcdf_write_hdr_system(self, iu, param) + implicit none + class(swiftest_nbody_system), intent(in) :: self !! Swiftest nbody system object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to for writing a NetCDF dataset to file + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine netcdf_write_hdr_system + + module subroutine netcdf_write_particle_info_base(self, iu) + implicit none + class(swiftest_base), intent(in) :: self !! Swiftest particle object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to identify a particular NetCDF dataset + end subroutine netcdf_write_particle_info_base + module subroutine obl_acc_body(self, system) implicit none class(swiftest_body), intent(inout) :: self !! Swiftest body object @@ -717,16 +928,10 @@ module subroutine obl_acc_tp(self, system) class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object end subroutine obl_acc_tp - module subroutine obl_pot(npl, Mcb, Mpl, j2rp2, j4rp4, xh, irh, oblpot) + module subroutine obl_pot_system(self) implicit none - integer(I4B), intent(in) :: npl - real(DP), intent(in) :: Mcb - real(DP), dimension(:), intent(in) :: Mpl - real(DP), intent(in) :: j2rp2, j4rp4 - real(DP), dimension(:), intent(in) :: irh - real(DP), dimension(:, :), intent(in) :: xh - real(DP), intent(out) :: oblpot - end subroutine obl_pot + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + end subroutine obl_pot_system module subroutine orbel_el2xv_vec(self, cb) implicit none @@ -761,6 +966,19 @@ module pure subroutine orbel_xv2aqt(mu, x, v, a, q, capm, tperi) real(DP), intent(out) :: tperi !! time of pericenter passage end subroutine orbel_xv2aqt + module pure subroutine orbel_xv2el(mu, x, v, a, e, inc, capom, omega, capm) + implicit none + real(DP), intent(in) :: mu !! Gravitational constant + real(DP), dimension(:), intent(in) :: x !! Position vector + real(DP), dimension(:), intent(in) :: v !! Velocity vector + real(DP), intent(out) :: a !! semimajor axis + real(DP), intent(out) :: e !! eccentricity + real(DP), intent(out) :: inc !! inclination + real(DP), intent(out) :: capom !! longitude of ascending node + real(DP), intent(out) :: omega !! argument of periapsis + real(DP), intent(out) :: capm !! mean anomaly + end subroutine orbel_xv2el + module subroutine orbel_xv2el_vec(self, cb) implicit none class(swiftest_body), intent(inout) :: self !! Swiftest body object @@ -777,7 +995,7 @@ end subroutine setup_body module subroutine setup_construct_system(system, param) implicit none class(swiftest_nbody_system), allocatable, intent(inout) :: system !! Swiftest system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters end subroutine setup_construct_system module subroutine setup_encounter(self, n) @@ -786,6 +1004,12 @@ module subroutine setup_encounter(self, n) integer(I4B), intent(in) :: n !! Number of encounters to allocate space for end subroutine setup_encounter + module subroutine setup_initialize_particle_info_system(self, param) + implicit none + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + end subroutine setup_initialize_particle_info_system + module subroutine setup_initialize_system(self, param) implicit none class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object @@ -794,8 +1018,8 @@ end subroutine setup_initialize_system module subroutine setup_pl(self, n, param) implicit none - class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object - integer(I4B), intent(in) :: n !! Number of particles to allocate space for + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + integer(I4B), intent(in) :: n !! Number of particles to allocate space for class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine setup_pl @@ -863,6 +1087,14 @@ module subroutine util_append_arr_I4B(arr, source, nold, nsrc, lsource_mask) logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to end subroutine util_append_arr_I4B + module subroutine util_append_arr_info(arr, source, nold, nsrc, lsource_mask) + implicit none + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array + type(swiftest_particle_info), dimension(:), allocatable, intent(in) :: source !! Array to append + integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + end subroutine util_append_arr_info + module subroutine util_append_arr_logical(arr, source, nold, nsrc, lsource_mask) implicit none logical, dimension(:), allocatable, intent(inout) :: arr !! Destination array @@ -875,11 +1107,18 @@ end subroutine util_append_arr_logical interface module subroutine util_append_body(self, source, lsource_mask) implicit none - class(swiftest_body), intent(inout) :: self !! Swiftest body object - class(swiftest_body), intent(in) :: source !! Source object to append + class(swiftest_body), intent(inout) :: self !! Swiftest body object + class(swiftest_body), intent(in) :: source !! Source object to append logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to end subroutine util_append_body + module subroutine util_append_encounter(self, source, lsource_mask) + implicit none + class(swiftest_encounter), intent(inout) :: self !! Swiftest encounter list object + class(swiftest_encounter), intent(in) :: source !! Source object to append + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + end subroutine util_append_encounter + module subroutine util_append_pl(self, source, lsource_mask) implicit none class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object @@ -918,12 +1157,61 @@ module subroutine util_coord_h2b_tp(self, cb) class(swiftest_cb), intent(in) :: cb !! Swiftest central body object end subroutine util_coord_h2b_tp + module subroutine util_coord_vb2vh_pl(self, cb) + implicit none + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + end subroutine util_coord_vb2vh_pl + + module subroutine util_coord_vb2vh_tp(self, vbcb) + implicit none + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body + end subroutine util_coord_vb2vh_tp + + module subroutine util_coord_vh2vb_pl(self, cb) + implicit none + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + end subroutine util_coord_vh2vb_pl + + module subroutine util_coord_vh2vb_tp(self, vbcb) + implicit none + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body + end subroutine util_coord_vh2vb_tp + + module subroutine util_coord_xh2xb_pl(self, cb) + implicit none + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + end subroutine util_coord_xh2xb_pl + + module subroutine util_coord_xh2xb_tp(self, cb) + implicit none + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + class(swiftest_cb), intent(in) :: cb !! Swiftest central body object + end subroutine util_coord_xh2xb_tp + module subroutine util_copy_encounter(self, source) implicit none class(swiftest_encounter), intent(inout) :: self !! Encounter list class(swiftest_encounter), intent(in) :: source !! Source object to copy into end subroutine util_copy_encounter + module subroutine util_copy_particle_info(self, source) + implicit none + class(swiftest_particle_info), intent(inout) :: self + class(swiftest_particle_info), intent(in) :: source + end subroutine util_copy_particle_info + + module subroutine util_copy_particle_info_arr(source, dest, idx) + implicit none + class(swiftest_particle_info), dimension(:), intent(in) :: source !! Source object to copy into + class(swiftest_particle_info), dimension(:), intent(inout) :: dest !! Swiftest body object with particle metadata information object + integer(I4B), dimension(:), intent(in), optional :: idx !! Optional array of indices to draw the source object + end subroutine util_copy_particle_info_arr + module subroutine util_exit(code) implicit none integer(I4B), intent(in) :: code !! Failure exit code @@ -980,6 +1268,13 @@ module subroutine util_fill_arr_I4B(keeps, inserts, lfill_list) logical, dimension(:), intent(in) :: lfill_list !! Logical array of bodies to merge into the keeps end subroutine util_fill_arr_I4B + module subroutine util_fill_arr_info(keeps, inserts, lfill_list) + implicit none + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + type(swiftest_particle_info), dimension(:), allocatable, intent(in) :: inserts !! Array of values to insert into keep + logical, dimension(:), intent(in) :: lfill_list !! Logical array of bodies to merge into the keeps + end subroutine util_fill_arr_info + module subroutine util_fill_arr_logical(keeps, inserts, lfill_list) implicit none logical, dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep @@ -996,7 +1291,7 @@ module subroutine util_rescale_system(self, param, mscale, dscale, tscale) real(DP), intent(in) :: mscale, dscale, tscale !! Scale factors for mass, distance, and time units, respectively. end subroutine util_rescale_system - module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) + module function util_minimize_bfgs(f, N, x0, eps, maxloop, lerr) result(x1) use lambda_function implicit none integer(I4B), intent(in) :: N @@ -1004,7 +1299,8 @@ module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) real(DP), dimension(:), intent(in) :: x0 real(DP), intent(in) :: eps logical, intent(out) :: lerr - real(DP), dimension(:), allocatable :: x1 + integer(I4B), intent(in) :: maxloop + real(DP), dimension(:), allocatable :: x1 end function util_minimize_bfgs module subroutine util_peri_tp(self, system, param) @@ -1041,6 +1337,12 @@ module subroutine util_resize_arr_I4B(arr, nnew) integer(I4B), intent(in) :: nnew !! New size end subroutine util_resize_arr_I4B + module subroutine util_resize_arr_info(arr, nnew) + implicit none + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Array to resize + integer(I4B), intent(in) :: nnew !! New size + end subroutine util_resize_arr_info + module subroutine util_resize_arr_logical(arr, nnew) implicit none logical, dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -1109,6 +1411,22 @@ module subroutine util_set_mu_tp(self, cb) class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object end subroutine util_set_mu_tp + module subroutine util_set_particle_info(self, name, particle_type, status, origin_type, origin_time, origin_xh, origin_vh, discard_time, discard_xh, discard_vh, discard_body_id) + implicit none + class(swiftest_particle_info), intent(inout) :: self + character(len=*), intent(in), optional :: name !! Non-unique name + character(len=*), intent(in), optional :: particle_type !! String containing a description of the particle type (e.g. Central Body, Massive Body, Test Particle) + character(len=*), intent(in), optional :: status !! Particle status description: Active, Merged, Fragmented, etc. + character(len=*), intent(in), optional :: origin_type !! String containing a description of the origin of the particle (e.g. Initial Conditions, Supercatastrophic, Disruption, etc.) + real(DP), intent(in), optional :: origin_time !! The time of the particle's formation + real(DP), dimension(:), intent(in), optional :: origin_xh !! The heliocentric distance vector at the time of the particle's formation + real(DP), dimension(:), intent(in), optional :: origin_vh !! The heliocentric velocity vector at the time of the particle's formation + real(DP), intent(in), optional :: discard_time !! The time of the particle's discard + real(DP), dimension(:), intent(in), optional :: discard_xh !! The heliocentric distance vector at the time of the particle's discard + real(DP), dimension(:), intent(in), optional :: discard_vh !! The heliocentric velocity vector at the time of the particle's discard + integer(I4B), intent(in), optional :: discard_body_id !! The id of the other body involved in the discard (0 if no other body involved) + end subroutine util_set_particle_info + module subroutine util_set_rhill(self,cb) implicit none class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object @@ -1190,6 +1508,50 @@ module subroutine util_sort_index_dp(arr,ind) end subroutine util_sort_index_dp end interface util_sort + interface util_sort_rearrange + module subroutine util_sort_rearrange_arr_char_string(arr, ind, n) + implicit none + character(len=STRMAX), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_char_string + + module subroutine util_sort_rearrange_arr_DP(arr, ind, n) + implicit none + real(DP), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_DP + + module subroutine util_sort_rearrange_arr_DPvec(arr, ind, n) + implicit none + real(DP), dimension(:,:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_DPvec + + module subroutine util_sort_rearrange_arr_I4B(arr, ind, n) + implicit none + integer(I4B), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_I4B + + module subroutine util_sort_rearrange_arr_info(arr, ind, n) + implicit none + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_info + + module subroutine util_sort_rearrange_arr_logical(arr, ind, n) + implicit none + logical, dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine util_sort_rearrange_arr_logical + end interface util_sort_rearrange + interface module subroutine util_sort_rearrange_body(self, ind) implicit none @@ -1264,6 +1626,22 @@ module subroutine util_spill_arr_I4B(keeps, discards, lspill_list, ldestructive) logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not end subroutine util_spill_arr_I4B + module subroutine util_spill_arr_I8B(keeps, discards, lspill_list, ldestructive) + implicit none + integer(I8B), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + integer(I8B), dimension(:), allocatable, intent(inout) :: discards !! Array of discards + logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss + logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + end subroutine util_spill_arr_I8B + + module subroutine util_spill_arr_info(keeps, discards, lspill_list, ldestructive) + implicit none + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: discards !! Array of discards + logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss + logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + end subroutine util_spill_arr_info + module subroutine util_spill_arr_logical(keeps, discards, lspill_list, ldestructive) implicit none logical, dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep @@ -1309,7 +1687,7 @@ end subroutine util_spill_tp module subroutine util_valid_id_system(self, param) implicit none class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters end subroutine util_valid_id_system module subroutine util_version() diff --git a/src/modules/swiftest_globals.f90 b/src/modules/swiftest_globals.f90 index 5ec55f6c6..1f9c6028c 100644 --- a/src/modules/swiftest_globals.f90 +++ b/src/modules/swiftest_globals.f90 @@ -22,7 +22,10 @@ module swiftest_globals real(DP), parameter :: PI3BY2 = 4.712388980384689857693965074919254326296_DP !! Definition of /(3 \pi / 2\) real(DP), parameter :: TWOPI = 6.283185307179586476925286766559005768394_DP !! Definition of 2 \pi real(DP), parameter :: THIRD = 0.333333333333333333333333333333333333333_DP !! Definition of 1 / 3 - real(DP), parameter :: DEGRAD = 180.0_DP/PI !! Definition of conversion factor from degrees to radians + real(DP), parameter :: DEG2RAD = PI / 180.0_DP !! Definition of conversion factor from degrees to radians + real(DP), parameter :: RAD2DEG = 180.0_DP / PI !! Definition of conversion factor from degrees to radians + real(DP), parameter :: GC = 6.6743E-11_DP !! Universal gravitational constant in SI units + real(DP), parameter :: einsteinC = 299792458.0_DP !! Speed of light in SI units integer(I4B), parameter :: LOWERCASE_BEGIN = iachar('a') !! ASCII character set parameter for lower to upper conversion - start of lowercase integer(I4B), parameter :: LOWERCASE_END = iachar('z') !! ASCII character set parameter for lower to upper conversion - end of lowercase @@ -41,16 +44,23 @@ module swiftest_globals integer(I4B), parameter :: SYMBA = 8 integer(I4B), parameter :: RINGMOONS = 9 - integer(I4B), parameter :: STRMAX = 128 !! Maximum size of character strings + integer(I4B), parameter :: STRMAX = 512 !! Maximum size of character strings + integer(I4B), parameter :: NAMELEN = 32 !! Maximum size of name strings character(*), parameter :: ASCII_TYPE = 'ASCII' !! Symbolic name for ASCII file type character(*), parameter :: REAL4_TYPE = 'REAL4' !! Symbolic name for binary file type REAL4 character(*), parameter :: REAL8_TYPE = 'REAL8' !! Symbolic name for binary file type REAL8 - character(*), parameter :: SWIFTER_REAL4_TYPE = 'SWIFTER4' !! Symbolic name for binary file type for the old style Swifter REAL4 - character(*), parameter :: SWIFTER_REAL8_TYPE = 'SWIFTER8' !! Symbolic name for binary file type for the old style Swifter REAL8 + character(*), parameter :: NETCDF_FLOAT_TYPE = 'NETCDF_FLOAT' !! Symbolic name for binary file type REAL8 + character(*), parameter :: NETCDF_DOUBLE_TYPE = 'NETCDF_DOUBLE' !! Symbolic name for binary file type REAL8 + + character(*), parameter :: EL = 'EL' !! Symbolic name for binary output file contents for orbital elements + character(*), parameter :: XV = 'XV' !! Symbolic name for binary output file contents for cartesian position and velocity vectors + character(*), parameter :: XVEL = 'XVEL' !! Symbolic name for binary output file contents for both cartesian position and velocity and orbital elements - character(*), parameter :: EL = 'EL' !! Symbolic name for binary output file contents for orbital element type - character(*), parameter :: XV = 'XV' !! Symbolic name for binary output file contents for cartesian position and velocity type + character(*), parameter :: CB_TYPE_NAME = "Central Body" + character(*), parameter :: PL_TYPE_NAME = "Massive Body" + character(*), parameter :: TP_TYPE_NAME = "Test Particle" + character(*), parameter :: PL_TINY_TYPE_NAME = "Semi-Interacting Massive Body" ! OpenMP Parameters integer(I4B) :: nthreads = 1 !! Number of OpenMP threads @@ -61,7 +71,6 @@ module swiftest_globals integer(I4B), parameter :: USAGE = -2 !! Symbolic name for function return/flag code for printing the usage message integer(I4B), parameter :: HELP = -3 !! Symbolic name for function return/flag code for printing the usage message - character(*), parameter :: SUCCESS_MSG = '(/, "Normal termination of Swiftest (version ", f3.1, ")")' character(*), parameter :: FAIL_MSG = '(/, "Terminating Swiftest (version ", f3.1, ") due to error!!")' character(*), parameter :: USAGE_MSG = '("Usage: swiftest [bs|helio|ra15|rmvs|symba|tu4|whm] ")' @@ -72,21 +81,24 @@ module swiftest_globals integer(I4B), parameter :: HYPERBOLA = 1 !! Symbolic names for orbit types - hyperbola !> Symbolic names for body/particle status codes: - integer(I4B), parameter :: ACTIVE = 0 - integer(I4B), parameter :: INACTIVE = 1 - integer(I4B), parameter :: DISCARDED_RMAX = -1 - integer(I4B), parameter :: DISCARDED_RMIN = -2 - integer(I4B), parameter :: DISCARDED_RMAXU = -3 - integer(I4B), parameter :: DISCARDED_PERI = -4 - integer(I4B), parameter :: DISCARDED_PLR = -5 - integer(I4B), parameter :: DISCARDED_PLQ = -6 - integer(I4B), parameter :: DISCARDED_DRIFTERR = -7 - integer(I4B), parameter :: MERGED = -8 - integer(I4B), parameter :: DISRUPTION = -9 - integer(I4B), parameter :: SUPERCATASTROPHIC = -10 - integer(I4B), parameter :: GRAZE_AND_MERGE = -11 - integer(I4B), parameter :: HIT_AND_RUN = -12 - integer(I4B), parameter :: COLLISION = -13 + integer(I4B), parameter :: ACTIVE = 0 + integer(I4B), parameter :: INACTIVE = 1 + integer(I4B), parameter :: DISCARDED_RMAX = -1 + integer(I4B), parameter :: DISCARDED_RMIN = -2 + integer(I4B), parameter :: DISCARDED_RMAXU = -3 + integer(I4B), parameter :: DISCARDED_PERI = -4 + integer(I4B), parameter :: DISCARDED_PLR = -5 + integer(I4B), parameter :: DISCARDED_PLQ = -6 + integer(I4B), parameter :: DISCARDED_DRIFTERR = -7 + integer(I4B), parameter :: MERGED = -8 + integer(I4B), parameter :: DISRUPTION = -9 + integer(I4B), parameter :: SUPERCATASTROPHIC = -10 + integer(I4B), parameter :: GRAZE_AND_MERGE = -11 + integer(I4B), parameter :: HIT_AND_RUN_DISRUPT = -12 + integer(I4B), parameter :: HIT_AND_RUN_PURE = -13 + integer(I4B), parameter :: COLLISION = -14 + integer(I4B), parameter :: NEW_PARTICLE = -15 + integer(I4B), parameter :: OLD_PARTICLE = -16 !>Symbolic names for collisional outcomes from collresolve_resolve: integer(I4B), parameter :: COLLRESOLVE_REGIME_MERGE = 1 @@ -104,24 +116,85 @@ module swiftest_globals character(*), dimension(2), parameter :: DUMP_CB_FILE = ['dump_cb1.bin', 'dump_cb2.bin' ] character(*), dimension(2), parameter :: DUMP_PL_FILE = ['dump_pl1.bin', 'dump_pl2.bin' ] character(*), dimension(2), parameter :: DUMP_TP_FILE = ['dump_tp1.bin', 'dump_tp2.bin' ] - character(*), dimension(2), parameter :: DUMP_PARAM_FILE = ['dump_param1.dat', 'dump_param2.dat'] + character(*), dimension(2), parameter :: DUMP_PARAM_FILE = ['dump_param1.in', 'dump_param2.in'] !> Default file names that can be changed by the user in the parameters file - character(*), parameter :: ENC_OUTFILE = 'encounter.out' - character(*), parameter :: DISCARD_FILE = 'discard.out' - character(*), parameter :: ENERGY_FILE = 'energy.out' - character(*), parameter :: CB_INFILE = 'cb.in' - character(*), parameter :: PL_INFILE = 'pl.in' - character(*), parameter :: TP_INFILE = 'tp.in' - character(*), parameter :: BIN_OUTFILE = 'bin.dat' - integer(I4B), parameter :: BINUNIT = 20 !! File unit number for the binary output file + character(*), parameter :: CB_INFILE = 'cb.in' + character(*), parameter :: PL_INFILE = 'pl.in' + character(*), parameter :: TP_INFILE = 'tp.in' + character(*), parameter :: BIN_OUTFILE = 'bin.dat' + integer(I4B), parameter :: BINUNIT = 20 !! File unit number for the binary output file + character(*), parameter :: PARTICLE_OUTFILE = 'particle.dat' + integer(I4B), parameter :: PARTICLEUNIT = 44 !! File unit number for the binary particle info output file !> Miscellaneous constants: integer(I4B), parameter :: NDIM = 3 !! Number of dimensions in our reality integer(I4B), parameter :: NDIM2 = 2 * NDIM !! 2x the number of dimensions real(DP), parameter :: VSMALL = 2 * epsilon(1._DP) !! Very small number used to prevent floating underflow - real(DP), parameter :: GC = 6.6743E-11_DP !! Universal gravitational constant in SI units - real(DP), parameter :: einsteinC = 299792458.0_DP !! Speed of light in SI units + !> NetCDF variable names and constants + character(*), parameter :: NETCDF_OUTFILE = 'bin.nc' !! Default output file name + character(*), parameter :: TIME_DIMNAME = "time" !! NetCDF name of the time dimension + character(*), parameter :: ID_DIMNAME = "id" !! NetCDF name of the particle id dimension + character(*), parameter :: STR_DIMNAME = "str" !! NetCDF name of the particle id dimension + character(*), parameter :: PTYPE_VARNAME = "particle_type" !! NetCDF name of the particle type variable + character(*), parameter :: NAME_VARNAME = "name" !! NetCDF name of the particle name variable + character(*), parameter :: NPL_VARNAME = "npl" !! NetCDF name of the number of active massive bodies variable + character(*), parameter :: NTP_VARNAME = "ntp" !! NetCDF name of the number of active test particles variable + character(*), parameter :: A_VARNAME = "a" !! NetCDF name of the semimajor axis variable + character(*), parameter :: E_VARNAME = "e" !! NetCDF name of the eccentricity variable + character(*), parameter :: INC_VARNAME = "inc" !! NetCDF name of the inclination variable + character(*), parameter :: CAPOM_VARNAME = "capom" !! NetCDF name of the long. asc. node variable + character(*), parameter :: OMEGA_VARNAME = "omega" !! NetCDF name of the arg. periapsis variable + character(*), parameter :: CAPM_VARNAME = "capm" !! NetCDF name of the mean anomaly variable + character(*), parameter :: XHX_VARNAME = "xhx" !! NetCDF name of the heliocentric position x variable + character(*), parameter :: XHY_VARNAME = "xhy" !! NetCDF name of the heliocentric position y variable + character(*), parameter :: XHZ_VARNAME = "xhz" !! NetCDF name of the heliocentric position z variable + character(*), parameter :: VHX_VARNAME = "vhx" !! NetCDF name of the heliocentric velocity x variable + character(*), parameter :: VHY_VARNAME = "vhy" !! NetCDF name of the heliocentric velocity y variable + character(*), parameter :: VHZ_VARNAME = "vhz" !! NetCDF name of the heliocentric velocity z variable + character(*), parameter :: GMASS_VARNAME = "Gmass" !! NetCDF name of the mass variable + character(*), parameter :: RHILL_VARNAME = "rhill" !! NetCDF name of the hill radius variable + character(*), parameter :: RADIUS_VARNAME = "radius" !! NetCDF name of the radius variable + character(*), parameter :: IP1_VARNAME = "Ip1" !! NetCDF name of the axis 1 principal moment of inertial variable + character(*), parameter :: IP2_VARNAME = "Ip2" !! NetCDF name of the axis 2 principal moment of inertial variable + character(*), parameter :: IP3_VARNAME = "Ip3" !! NetCDF name of the axis 3 principal moment of inertial variable + character(*), parameter :: ROTX_VARNAME = "rotx" !! NetCDF name of the rotation x variable + character(*), parameter :: ROTY_VARNAME = "roty" !! NetCDF name of the rotation y variable + character(*), parameter :: ROTZ_VARNAME = "rotz" !! NetCDF name of the rotation z variable + character(*), parameter :: K2_VARNAME = "k2" !! NetCDF name of the Love number variable + character(*), parameter :: Q_VARNAME = "Q" !! NetCDF name of the energy dissipation variable + character(*), parameter :: KE_ORB_VARNAME = "KE_orb" !! NetCDF name of the system orbital kinetic energy variable + character(*), parameter :: KE_SPIN_VARNAME = "KE_spin" !! NetCDF name of the system spin kinetic energy variable + character(*), parameter :: PE_VARNAME = "PE" !! NetCDF name of the system potential energy variable + character(*), parameter :: L_ORBX_VARNAME = "L_orbx" !! NetCDF name of the orbital angular momentum x variable + character(*), parameter :: L_ORBY_VARNAME = "L_orby" !! NetCDF name of the orbital angular momentum y variable + character(*), parameter :: L_ORBZ_VARNAME = "L_orbz" !! NetCDF name of the orbital angular momentum z variable + character(*), parameter :: L_SPINX_VARNAME = "L_spinx" !! NetCDF name of the spin angular momentum x variable + character(*), parameter :: L_SPINY_VARNAME = "L_spiny" !! NetCDF name of the spin angular momentum y variable + character(*), parameter :: L_SPINZ_VARNAME = "L_spinz" !! NetCDF name of the spin angular momentum z variable + character(*), parameter :: L_ESCAPEX_VARNAME = "L_escapex" !! NetCDF name of the escaped angular momentum x variable + character(*), parameter :: L_ESCAPEY_VARNAME = "L_escapey" !! NetCDF name of the escaped angular momentum y variable + character(*), parameter :: L_ESCAPEZ_VARNAME = "L_escapez" !! NetCDF name of the escaped angular momentum z variable + character(*), parameter :: ECOLLISIONS_VARNAME = "Ecollisions" !! NetCDF name of the escaped angular momentum y variable + character(*), parameter :: EUNTRACKED_VARNAME = "Euntracked" !! NetCDF name of the energy that is untracked due to loss (untracked potential energy due to mergers and body energy for escaped bodies) + character(*), parameter :: GMESCAPE_VARNAME = "GMescape" !! NetCDF name of the G*Mass of bodies that escape the system + character(*), parameter :: STATUS_VARNAME = "status" !! NetCDF name of the current status of the body variable (includes discard type) + character(*), parameter :: ORIGIN_TYPE_VARNAME = "origin_type" !! NetCDF name of the origin type variable (Initial Conditions, Disruption, etc.) + character(*), parameter :: ORIGIN_TIME_VARNAME = "origin_time" !! NetCDF name of the time of origin variable + character(*), parameter :: ORIGIN_XHX_VARNAME = "origin_xhx" !! NetCDF name of the heliocentric position of the body at the time of origin x variable + character(*), parameter :: ORIGIN_XHY_VARNAME = "origin_xhy" !! NetCDF name of the heliocentric position of the body at the time of origin y variable + character(*), parameter :: ORIGIN_XHZ_VARNAME = "origin_xhz" !! NetCDF name of the heliocentric position of the body at the time of origin z variable + character(*), parameter :: ORIGIN_VHX_VARNAME = "origin_vhx" !! NetCDF name of the heliocentric velocity of the body at the time of origin x variable + character(*), parameter :: ORIGIN_VHY_VARNAME = "origin_vhy" !! NetCDF name of the heliocentric velocity of the body at the time of origin y variable + character(*), parameter :: ORIGIN_VHZ_VARNAME = "origin_vhz" !! NetCDF name of the heliocentric velocity of the body at the time of origin z variable + character(*), parameter :: DISCARD_TIME_VARNAME = "discard_time" !! NetCDF name of the time of discard variable + character(*), parameter :: DISCARD_XHX_VARNAME = "discard_xhx" !! NetCDF name of the heliocentric position of the body at the time of discard x variable + character(*), parameter :: DISCARD_XHY_VARNAME = "discard_xhy" !! NetCDF name of the heliocentric position of the body at the time of discard y variable + character(*), parameter :: DISCARD_XHZ_VARNAME = "discard_xhz" !! NetCDF name of the heliocentric position of the body at the time of discard z variable + character(*), parameter :: DISCARD_VHX_VARNAME = "discard_vhx" !! NetCDF name of the heliocentric velocity of the body at the time of discard x variable + character(*), parameter :: DISCARD_VHY_VARNAME = "discard_vhy" !! NetCDF name of the heliocentric velocity of the body at the time of discard y variable + character(*), parameter :: DISCARD_VHZ_VARNAME = "discard_vhz" !! NetCDF name of the heliocentric velocity of the body at the time of discard z variable + character(*), parameter :: DISCARD_BODY_ID_VARNAME = "discard_body_id" !! NetCDF name of the id of the other body involved in the discard end module swiftest_globals diff --git a/src/modules/symba_classes.f90 b/src/modules/symba_classes.f90 index 4628202f8..21986b920 100644 --- a/src/modules/symba_classes.f90 +++ b/src/modules/symba_classes.f90 @@ -1,12 +1,13 @@ module symba_classes !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! - !! Definition of classes and methods specific to the Democratic SyMBAcentric Method - !! Adapted from David E. Kaufmann's Swifter routine: helio.f90 + !! Definition of classes and methods specific to the SyMBA integrator + !! Adapted from David E. Kaufmann's Swifter routine: module_symba.f90 use swiftest_globals - use swiftest_classes, only : swiftest_parameters, swiftest_base, swiftest_encounter + use swiftest_classes, only : swiftest_parameters, swiftest_base, swiftest_encounter, swiftest_particle_info, netcdf_parameters use helio_classes, only : helio_cb, helio_pl, helio_tp, helio_nbody_system use rmvs_classes, only : rmvs_chk_ind + use fraggle_classes, only : fraggle_colliders, fraggle_fragments implicit none public @@ -14,32 +15,17 @@ module symba_classes integer(I4B), private, parameter :: NTENC = 3 real(DP), private, parameter :: RHSCALE = 6.5_DP real(DP), private, parameter :: RSHELL = 0.48075_DP - character(*), parameter :: PARTICLE_OUTFILE = 'particle.dat' - integer(I4B), parameter :: PARTICLEUNIT = 44 !! File unit number for the binary particle info output file type, extends(swiftest_parameters) :: symba_parameters - character(STRMAX) :: particle_out = PARTICLE_OUTFILE !! Name of output particle information file - real(DP) :: GMTINY = -1.0_DP !! Smallest mass that is fully gravitating - integer(I4B), dimension(:), allocatable :: seed !! Random seeds - logical :: lfragmentation = .false. !! Do fragmentation modeling instead of simple merger. + real(DP) :: GMTINY = -1.0_DP !! Smallest G*mass that is fully gravitating + real(DP) :: min_GMfrag = -1.0_DP !! Smallest G*mass that can be produced in a fragmentation event + integer(I4B), dimension(:), allocatable :: seed !! Random seeds + logical :: lfragmentation = .false. !! Do fragmentation modeling instead of simple merger. contains procedure :: reader => symba_io_param_reader procedure :: writer => symba_io_param_writer end type symba_parameters - !******************************************************************************************************************************** - ! symba_particle_info class definitions and method interfaces - !******************************************************************************************************************************* - !> Class definition for the particle origin information object. This object is used to track time, location, and collisional regime - !> of fragments produced in collisional events. - type :: symba_particle_info - sequence - character(len=32) :: origin_type !! String containing a description of the origin of the particle (e.g. Initial Conditions, Supercatastrophic, Disruption, etc.) - real(DP) :: origin_time !! The time of the particle's formation - real(DP), dimension(NDIM) :: origin_xh !! The heliocentric distance vector at the time of the particle's formation - real(DP), dimension(NDIM) :: origin_vh !! The heliocentric velocity vector at the time of the particle's formation - end type symba_particle_info - !******************************************************************************************************************************** ! symba_kinship class definitions and method interfaces !******************************************************************************************************************************* @@ -55,11 +41,10 @@ module symba_classes !******************************************************************************************************************************* !> SyMBA central body particle class type, extends(helio_cb) :: symba_cb - real(DP) :: M0 = 0.0_DP !! Initial mass of the central body - real(DP) :: dM = 0.0_DP !! Change in mass of the central body + real(DP) :: GM0 = 0.0_DP !! Initial G*mass of the central body + real(DP) :: dGM = 0.0_DP !! Change in G*mass of the central body real(DP) :: R0 = 0.0_DP !! Initial radius of the central body real(DP) :: dR = 0.0_DP !! Change in the radius of the central body - type(symba_particle_info) :: info contains end type symba_cb @@ -81,18 +66,20 @@ module symba_classes real(DP), dimension(:), allocatable :: peri !! perihelion distance real(DP), dimension(:), allocatable :: atp !! semimajor axis following perihelion passage type(symba_kinship), dimension(:), allocatable :: kin !! Array of merger relationship structures that can account for multiple pairwise mergers in a single step - type(symba_particle_info), dimension(:), allocatable :: info contains - procedure :: make_family => symba_collision_make_family_pl !! When a single body is involved in more than one collision in a single step, it becomes part of a family + procedure :: make_colliders => symba_collision_make_colliders_pl !! When a single body is involved in more than one collision in a single step, it becomes part of a family + procedure :: index => symba_util_index_eucl_plpl !! Sets up the (i, j) -> k indexing used for the single-loop blocking Euclidean distance matrix procedure :: discard => symba_discard_pl !! Process massive body discards procedure :: drift => symba_drift_pl !! Method for Danby drift in Democratic Heliocentric coordinates. Sets the mask to the current recursion level procedure :: encounter_check => symba_encounter_check_pl !! Checks if massive bodies are going through close encounters with each other + procedure :: accel_int => symba_kick_getacch_int_pl !! Compute direct cross (third) term heliocentric accelerations of massive bodiess, with no mutual interactions between bodies below GMTINY procedure :: accel => symba_kick_getacch_pl !! Compute heliocentric accelerations of massive bodies procedure :: setup => symba_setup_pl !! Constructor method - Allocates space for the input number of bodies procedure :: append => symba_util_append_pl !! Appends elements from one structure to another procedure :: fill => symba_util_fill_pl !! "Fills" bodies from one object into another depending on the results of a mask (uses the UNPACK intrinsic) procedure :: get_peri => symba_util_peri_pl !! Determine system pericenter passages for massive bodies procedure :: rearray => symba_util_rearray_pl !! Clean up the massive body structures to remove discarded bodies and add new bodies + procedure :: reset_kinship => symba_util_reset_kinship !! Resets the kinship status of bodies procedure :: resize => symba_util_resize_pl !! Checks the current size of a SyMBA massive body against the requested size and resizes it if it is too small. procedure :: sort => symba_util_sort_pl !! Sorts body arrays by a sortable componen procedure :: rearrange => symba_util_sort_rearrange_pl !! Rearranges the order of array elements of body based on an input index array. Used in sorting methods @@ -115,7 +102,6 @@ module symba_classes integer(I4B), dimension(:), allocatable :: nplenc !! number of encounters with planets this time step integer(I4B), dimension(:), allocatable :: levelg !! level at which this particle should be moved integer(I4B), dimension(:), allocatable :: levelm !! deepest encounter level achieved this time step - type(symba_particle_info), dimension(:), allocatable :: info contains procedure :: drift => symba_drift_tp !! Method for Danby drift in Democratic Heliocentric coordinates. Sets the mask to the current recursion level procedure :: encounter_check => symba_encounter_check_tp !! Checks if any test particles are undergoing a close encounter with a massive body @@ -129,88 +115,122 @@ module symba_classes procedure :: spill => symba_util_spill_tp !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) end type symba_tp + !******************************************************************************************************************************** + ! symba_encounter class definitions and method interfaces + !******************************************************************************************************************************* + !> SyMBA class for tracking close encounters in a step + type, extends(swiftest_encounter) :: symba_encounter + integer(I4B), dimension(:), allocatable :: level !! encounter recursion level + contains + procedure :: collision_check => symba_collision_check_encounter !! Checks if a test particle is going to collide with a massive body + procedure :: encounter_check => symba_encounter_check !! Checks if massive bodies are going through close encounters with each other + procedure :: kick => symba_kick_encounter !! Kick barycentric velocities of active test particles within SyMBA recursion + procedure :: setup => symba_setup_encounter !! A constructor that sets the number of encounters and allocates and initializes all arrays + procedure :: copy => symba_util_copy_encounter !! Copies elements from the source encounter list into self. + procedure :: spill => symba_util_spill_encounter !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) + procedure :: append => symba_util_append_encounter !! Appends elements from one structure to another + end type symba_encounter + !******************************************************************************************************************************** ! symba_pltpenc class definitions and method interfaces !******************************************************************************************************************************* !> SyMBA class for tracking pl-tp close encounters in a step - type, extends(swiftest_encounter) :: symba_pltpenc - integer(I4B), dimension(:), allocatable :: level !! encounter recursion level + type, extends(symba_encounter) :: symba_pltpenc contains - procedure :: collision_check => symba_collision_check_pltpenc !! Checks if a test particle is going to collide with a massive body - procedure :: encounter_check => symba_encounter_check_pltpenc !! Checks if massive bodies are going through close encounters with each other - procedure :: kick => symba_kick_pltpenc !! Kick barycentric velocities of active test particles within SyMBA recursion - procedure :: setup => symba_setup_pltpenc !! A constructor that sets the number of encounters and allocates and initializes all arrays - procedure :: spill => symba_util_spill_pltpenc !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic) + procedure :: resolve_collision => symba_collision_resolve_pltpenc !! Process the pl-tp collision list, then modifiy the massive bodies based on the outcome of the c end type symba_pltpenc !******************************************************************************************************************************** ! symba_plplenc class definitions and method interfaces !******************************************************************************************************************************* !> SyMBA class for tracking pl-pl close encounters in a step - type, extends(symba_pltpenc) :: symba_plplenc + type, extends(symba_encounter) :: symba_plplenc contains - procedure :: scrub_non_collision => symba_collision_encounter_scrub !! Processes the pl-pl encounter list remove only those encounters that led to a collision - procedure :: resolve_fragmentations => symba_collision_resolve_fragmentations !! Process list of collisions, determine the collisional regime, and then create fragments - procedure :: resolve_mergers => symba_collision_resolve_mergers !! Process list of collisions and merge colliding bodies together + procedure :: extract_collisions => symba_collision_encounter_extract_collisions !! Processes the pl-pl encounter list remove only those encounters that led to a collision + procedure :: resolve_fragmentations => symba_collision_resolve_fragmentations !! Process list of collisions, determine the collisional regime, and then create fragments + procedure :: resolve_mergers => symba_collision_resolve_mergers !! Process list of collisions and merge colliding bodies together + procedure :: resolve_collision => symba_collision_resolve_plplenc !! Process the pl-pl collision list, then modifiy the massive bodies based on the outcome of the c end type symba_plplenc !******************************************************************************************************************************** ! symba_nbody_system class definitions and method interfaces !******************************************************************************************************************************** type, extends(helio_nbody_system) :: symba_nbody_system - class(symba_merger), allocatable :: pl_adds !! List of added bodies in mergers or collisions - class(symba_pltpenc), allocatable :: pltpenc_list !! List of massive body-test particle encounters in a single step - class(symba_plplenc), allocatable :: plplenc_list !! List of massive body-massive body encounters in a single step - integer(I4B) :: irec !! System recursion level + class(symba_merger), allocatable :: pl_adds !! List of added bodies in mergers or collisions + class(symba_pltpenc), allocatable :: pltpenc_list !! List of massive body-test particle encounters in a single step + class(symba_plplenc), allocatable :: plplenc_list !! List of massive body-massive body encounters in a single step + class(symba_plplenc), allocatable :: plplcollision_list !! List of massive body-massive body collisions in a single step + integer(I4B) :: irec !! System recursion level contains - procedure :: write_discard => symba_io_write_discard !! Write out information about discarded and merged planets and test particles in SyMBA - procedure :: initialize => symba_setup_initialize_system !! Performs SyMBA-specific initilization steps - procedure :: step => symba_step_system !! Advance the SyMBA nbody system forward in time by one step - procedure :: interp => symba_step_interp_system !! Perform an interpolation step on the SymBA nbody system - procedure :: set_recur_levels => symba_step_set_recur_levels_system !! Sets recursion levels of bodies and encounter lists to the current system level - procedure :: recursive_step => symba_step_recur_system !! Step interacting planets and active test particles ahead in democratic heliocentric coordinates at the current recursion level, if applicable, and descend to the next deeper level if necessary - procedure :: reset => symba_step_reset_system !! Resets pl, tp,and encounter structures at the start of a new step + procedure :: write_discard => symba_io_write_discard !! Write out information about discarded and merged planets and test particles in SyMBA + procedure :: initialize => symba_setup_initialize_system !! Performs SyMBA-specific initilization steps + procedure :: step => symba_step_system !! Advance the SyMBA nbody system forward in time by one step + procedure :: interp => symba_step_interp_system !! Perform an interpolation step on the SymBA nbody system + procedure :: set_recur_levels => symba_step_set_recur_levels_system !! Sets recursion levels of bodies and encounter lists to the current system level + procedure :: recursive_step => symba_step_recur_system !! Step interacting planets and active test particles ahead in democratic heliocentric coordinates at the current recursion level, if applicable, and descend to the next deeper level if necessary + procedure :: reset => symba_step_reset_system !! Resets pl, tp,and encounter structures at the start of a new step end type symba_nbody_system interface - module subroutine symba_collision_check_pltpenc(self, system, param, t, dt, irec) + module function symba_collision_check_encounter(self, system, param, t, dt, irec) result(lany_collision) use swiftest_classes, only : swiftest_parameters implicit none - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter list object - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - real(DP), intent(in) :: t !! current time - real(DP), intent(in) :: dt !! step size - integer(I4B), intent(in) :: irec !! Current recursion level - end subroutine symba_collision_check_pltpenc + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter list object + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! current time + real(DP), intent(in) :: dt !! step size + integer(I4B), intent(in) :: irec !! Current recursion level + logical :: lany_collision !! Returns true if cany pair of encounters resulted in a collision n + end function symba_collision_check_encounter - module subroutine symba_collision_encounter_scrub(self, system, param) + module subroutine symba_collision_encounter_extract_collisions(self, system, param) implicit none class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameterss + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine - module subroutine symba_collision_make_family_pl(self,idx) + module subroutine symba_collision_make_colliders_pl(self,idx) implicit none class(symba_pl), intent(inout) :: self !! SyMBA massive body object integer(I4B), dimension(2), intent(in) :: idx !! Array holding the indices of the two bodies involved in the collision - end subroutine symba_collision_make_family_pl + end subroutine symba_collision_make_colliders_pl module subroutine symba_collision_resolve_fragmentations(self, system, param) implicit none class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions end subroutine symba_collision_resolve_fragmentations module subroutine symba_collision_resolve_mergers(self, system, param) implicit none class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions end subroutine symba_collision_resolve_mergers + module subroutine symba_collision_resolve_plplenc(self, system, param, t, dt, irec) + implicit none + class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + real(DP), intent(in) :: t !! Current simulation time + real(DP), intent(in) :: dt !! Current simulation step size + integer(I4B), intent(in) :: irec !! Current recursion level + end subroutine symba_collision_resolve_plplenc + + module subroutine symba_collision_resolve_pltpenc(self, system, param, t, dt, irec) + implicit none + class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter list + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + real(DP), intent(in) :: t !! Current simulation time + real(DP), intent(in) :: dt !! Current simulation step size + integer(I4B), intent(in) :: irec !! Current recursion level + end subroutine symba_collision_resolve_pltpenc + module subroutine symba_discard_pl(self, system, param) use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters implicit none @@ -254,14 +274,14 @@ module function symba_encounter_check_pl(self, system, dt, irec) result(lany_enc logical :: lany_encounter !! Returns true if there is at least one close encounter end function symba_encounter_check_pl - module function symba_encounter_check_pltpenc(self, system, dt, irec) result(lany_encounter) + module function symba_encounter_check(self, system, dt, irec) result(lany_encounter) implicit none - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-pl encounter list object + class(symba_encounter), intent(inout) :: self !! SyMBA pl-pl encounter list object class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object real(DP), intent(in) :: dt !! step size integer(I4B), intent(in) :: irec !! Current recursion level logical :: lany_encounter !! Returns true if there is at least one close encounter - end function symba_encounter_check_pltpenc + end function symba_encounter_check module function symba_encounter_check_tp(self, system, dt, irec) result(lany_encounter) implicit none @@ -272,68 +292,43 @@ module function symba_encounter_check_tp(self, system, dt, irec) result(lany_enc logical :: lany_encounter !! Returns true if there is at least one close encounter end function symba_encounter_check_tp - module function symba_fragmentation_casedisruption(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collisionn - integer(I4B) :: status !! Status flag assigned to this outcome - end function symba_fragmentation_casedisruption + module function symba_collision_casedisruption(system, param, colliders, frag) result(status) + use fraggle_classes, only : fraggle_colliders, fraggle_fragments + implicit none + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + integer(I4B) :: status !! Status flag assigned to this outcome + end function symba_collision_casedisruption - module function symba_fragmentation_casehitandrun(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collision - integer(I4B) :: status !! Status flag assigned to this outcome - end function symba_fragmentation_casehitandrun - - module function symba_fragmentation_casemerge(system, param, family, x, v, mass, radius, L_spin, Ip) result(status) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(in) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(in) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collisio - integer(I4B) :: status !! Status flag assigned to this outcome - end function symba_fragmentation_casemerge - - module function symba_fragmentation_casesupercatastrophic(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collision - integer(I4B) :: status !! Status flag assigned to this outcome - end function symba_fragmentation_casesupercatastrophic - - module subroutine symba_io_write_discard(self, param) + module function symba_collision_casehitandrun(system, param, colliders, frag) result(status) + use fraggle_classes, only : fraggle_colliders, fraggle_fragments + implicit none + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + integer(I4B) :: status !! Status flag assigned to this outcome + end function symba_collision_casehitandrun + + module function symba_collision_casemerge(system, param, colliders, frag) result(status) + use fraggle_classes, only : fraggle_colliders, fraggle_fragments + implicit none + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + integer(I4B) :: status !! Status flag assigned to this outcome + end function symba_collision_casemerge + + module subroutine symba_util_index_eucl_plpl(self, param) use swiftest_classes, only : swiftest_parameters implicit none - class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - end subroutine symba_io_write_discard + class(symba_pl), intent(inout) :: self !! SyMBA massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine symba_util_index_eucl_plpl - module subroutine symba_io_dump_particle_info(system, param, lincludecb, tpidx, plidx) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA extensions - logical, optional, intent(in) :: lincludecb !! Set to true to include the central body (default is false) - integer(I4B), dimension(:), optional, intent(in) :: tpidx !! Array of test particle indices to append to the particle file - integer(I4B), dimension(:), optional, intent(in) :: plidx !! Array of massive body indices to append to the particle file - end subroutine symba_io_dump_particle_info - module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, iomsg) implicit none class(symba_parameters), intent(inout) :: self !! Current run configuration parameters with SyMBA additionss @@ -356,11 +351,17 @@ module subroutine symba_io_param_writer(self, unit, iotype, v_list, iostat, ioms character(len=*), intent(inout) :: iomsg !! Message to pass if iostat /= 0 end subroutine symba_io_param_writer - module subroutine symba_io_read_particle(system, param) + module subroutine symba_io_write_discard(self, param) + use swiftest_classes, only : swiftest_parameters + implicit none + class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + end subroutine symba_io_write_discard + + module subroutine symba_kick_getacch_int_pl(self) implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system file - class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA extensions - end subroutine symba_io_read_particle + class(symba_pl), intent(inout) :: self + end subroutine symba_kick_getacch_int_pl module subroutine symba_kick_getacch_pl(self, system, param, t, lbeg) use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters @@ -382,20 +383,14 @@ module subroutine symba_kick_getacch_tp(self, system, param, t, lbeg) logical, intent(in) :: lbeg !! Logical flag that determines whether or not this is the beginning or end of the step end subroutine symba_kick_getacch_tp - module subroutine symba_kick_pltpenc(self, system, dt, irec, sgn) + module subroutine symba_kick_encounter(self, system, dt, irec, sgn) implicit none - class(symba_pltpenc), intent(in) :: self !! SyMBA pl-tp encounter list object + class(symba_encounter), intent(in) :: self !! SyMBA pl-tp encounter list object class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object real(DP), intent(in) :: dt !! step size integer(I4B), intent(in) :: irec !! Current recursion level integer(I4B), intent(in) :: sgn !! sign to be applied to acceleration - end subroutine symba_kick_pltpenc - - module subroutine symba_setup_initialize_particle_info(system, param) - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA extensions - end subroutine symba_setup_initialize_particle_info + end subroutine symba_kick_encounter module subroutine symba_setup_initialize_system(self, param) use swiftest_classes, only : swiftest_parameters @@ -420,11 +415,11 @@ module subroutine symba_setup_pl(self, n, param) class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters end subroutine symba_setup_pl - module subroutine symba_setup_pltpenc(self,n) + module subroutine symba_setup_encounter(self,n) implicit none - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter structure + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter structure integer(I4B), intent(in) :: n !! Number of encounters to allocate space for - end subroutine symba_setup_pltpenc + end subroutine symba_setup_encounter module subroutine symba_setup_tp(self, n, param) use swiftest_classes, only : swiftest_parameters @@ -463,25 +458,18 @@ module recursive subroutine symba_step_recur_system(self, param, t, ireci) implicit none class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - real(DP), value :: t - integer(I4B), value :: ireci !! input recursion level + real(DP), intent(in) :: t + integer(I4B), intent(in) :: ireci !! input recursion level end subroutine symba_step_recur_system - module subroutine symba_step_reset_system(self) + module subroutine symba_step_reset_system(self, param) implicit none - class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object + class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object + class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions end subroutine symba_step_reset_system end interface interface util_append - module subroutine symba_util_append_arr_info(arr, source, nold, nsrc, lsource_mask) - implicit none - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array - type(symba_particle_info), dimension(:), allocatable, intent(in) :: source !! Array to append - integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively - logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to - end subroutine symba_util_append_arr_info - module subroutine symba_util_append_arr_kin(arr, source, nold, nsrc, lsource_mask) implicit none type(symba_kinship), dimension(:), allocatable, intent(inout) :: arr !! Destination array @@ -492,6 +480,13 @@ end subroutine symba_util_append_arr_kin end interface interface + module subroutine symba_util_append_encounter(self, source, lsource_mask) + implicit none + class(symba_encounter), intent(inout) :: self !! SyMBA encounter list object + class(swiftest_encounter), intent(in) :: source !! Source object to append + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + end subroutine symba_util_append_encounter + module subroutine symba_util_append_merger(self, source, lsource_mask) use swiftest_classes, only : swiftest_body implicit none @@ -515,16 +510,16 @@ module subroutine symba_util_append_tp(self, source, lsource_mask) class(swiftest_body), intent(in) :: source !! Source object to append logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to end subroutine symba_util_append_tp - end interface - interface util_fill - module subroutine symba_util_fill_arr_info(keeps, inserts, lfill_list) + module subroutine symba_util_copy_encounter(self, source) + use swiftest_classes, only : swiftest_encounter implicit none - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep - type(symba_particle_info), dimension(:), allocatable, intent(in) :: inserts !! Array of values to insert into keep - logical, dimension(:), intent(in) :: lfill_list !! Logical array of bodies to merge into the keeps - end subroutine symba_util_fill_arr_info + class(symba_encounter), intent(inout) :: self !! Encounter list + class(swiftest_encounter), intent(in) :: source !! Source object to copy into + end subroutine symba_util_copy_encounter + end interface + interface util_fill module subroutine symba_util_fill_arr_kin(keeps, inserts, lfill_list) implicit none type(symba_kinship), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep @@ -562,17 +557,19 @@ module subroutine symba_util_rearray_pl(self, system, param) implicit none class(symba_pl), intent(inout) :: self !! SyMBA massive body object class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions end subroutine symba_util_rearray_pl - end interface - interface util_resize - module subroutine symba_util_resize_arr_info(arr, nnew) + module subroutine symba_util_reset_kinship(self, idx) implicit none - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Array to resize - integer(I4B), intent(in) :: nnew !! New size - end subroutine symba_util_resize_arr_info + class(symba_pl), intent(inout) :: self !! SyMBA massive body object + integer(I4B), dimension(:), intent(in) :: idx !! Index array of bodies to reset + integer(I4B) :: i, j + end subroutine symba_util_reset_kinship + + end interface + interface util_resize module subroutine symba_util_resize_arr_kin(arr, nnew) implicit none type(symba_kinship), dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -612,7 +609,18 @@ module subroutine symba_util_sort_tp(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order end subroutine symba_util_sort_tp + end interface + + interface util_sort_rearrange + module subroutine symba_util_sort_rearrange_arr_kin(arr, ind, n) + implicit none + type(symba_kinship), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + end subroutine symba_util_sort_rearrange_arr_kin + end interface util_sort_rearrange + interface module subroutine symba_util_sort_rearrange_pl(self, ind) implicit none class(symba_pl), intent(inout) :: self !! SyMBA massive body object @@ -627,14 +635,6 @@ end subroutine symba_util_sort_rearrange_tp end interface interface util_spill - module subroutine symba_util_spill_arr_info(keeps, discards, lspill_list, ldestructive) - implicit none - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: discards !! Array of discards - logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss - logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not - end subroutine symba_util_spill_arr_info - module subroutine symba_util_spill_arr_kin(keeps, discards, lspill_list, ldestructive) implicit none type(symba_kinship), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep @@ -654,14 +654,14 @@ module subroutine symba_util_spill_pl(self, discards, lspill_list, ldestructive) logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not end subroutine symba_util_spill_pl - module subroutine symba_util_spill_pltpenc(self, discards, lspill_list, ldestructive) + module subroutine symba_util_spill_encounter(self, discards, lspill_list, ldestructive) use swiftest_classes, only : swiftest_encounter implicit none - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter list + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter list class(swiftest_encounter), intent(inout) :: discards !! Discarded object logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list - end subroutine symba_util_spill_pltpenc + end subroutine symba_util_spill_encounter module subroutine symba_util_spill_tp(self, discards, lspill_list, ldestructive) use swiftest_classes, only : swiftest_body diff --git a/src/modules/walltime_classes.f90 b/src/modules/walltime_classes.f90 new file mode 100644 index 000000000..6425b5b5f --- /dev/null +++ b/src/modules/walltime_classes.f90 @@ -0,0 +1,119 @@ +module walltime_classes + !! author: David A. Minton + !! + !! Classes and methods used to compute elasped wall time + use swiftest_globals + implicit none + public + + type :: walltimer + integer(I8B) :: count_rate !! Rate at wich the clock ticks + integer(I8B) :: count_max !! Maximum value of the clock ticker + integer(I8B) :: count_start_main !! Value of the clock ticker at when the timer is first called + integer(I8B) :: count_start_step !! Value of the clock ticker at the start of a timed step + integer(I8B) :: count_finish_step !! Value of the clock ticker at the end of a timed step + logical :: lmain_is_started = .false. !! Logical flag indicating whether or not the main timer has been reset or not + contains + procedure :: reset => walltime_reset !! Resets the clock ticker, settting main_start to the current ticker value + procedure :: start => walltime_start !! Starts the timer, setting step_start to the current ticker value + procedure :: finish => walltime_finish !! Ends the timer, setting step_finish to the current ticker value and printing the elapsed time information to the terminal + end type + + interface + module subroutine walltime_finish(self, nsubsteps, message) + implicit none + class(walltimer), intent(inout) :: self !! Walltimer object + integer(I4B), intent(in) :: nsubsteps !! Number of substeps used to compute the time per step + character(len=*), intent(in) :: message !! Message to prepend to the wall time terminal output + end subroutine walltime_finish + + module subroutine walltime_reset(self) + implicit none + class(walltimer), intent(inout) :: self !! Walltimer object + end subroutine walltime_reset + + module subroutine walltime_start(self) + implicit none + class(walltimer), intent(inout) :: self !! Walltimer object + end subroutine walltime_start + end interface + + contains + + module subroutine walltime_finish(self, nsubsteps, message) + !! author: David A. Minton + !! + !! Ends the timer, setting step_finish to the current ticker value and printing the elapsed time information to the terminal + use swiftest_globals + implicit none + ! Arguments + class(walltimer), intent(inout) :: self !! Walltimer object + integer(I4B), intent(in) :: nsubsteps !! Number of substeps used to compute the time per step + character(len=*), intent(in) :: message !! Message to prepend to the wall time terminal output + ! Internals + character(len=*), parameter :: walltimefmt = '" Wall time (s): ", es12.5, "; Wall time/step in this interval (s): ", es12.5' + character(len=STRMAX) :: fmt + integer(I8B) :: count_delta_step, count_delta_main + real(DP) :: wall_main !! Value of total elapsed time at the end of a timed step + real(DP) :: wall_step !! Value of elapsed time since the start of a timed step + real(DP) :: wall_per_substep !! Value of time per substep + + if (.not.self%lmain_is_started) then + write(*,*) "Wall timer error: The step finish time cannot be calculated because the timer is not started!" + return + end if + + call system_clock(self%count_finish_step) + + count_delta_step = self%count_finish_step - self%count_start_step + count_delta_main = self%count_finish_step - self%count_start_main + wall_step = count_delta_step / (self%count_rate * 1.0_DP) + wall_main = count_delta_main / (self%count_rate * 1.0_DP) + wall_per_substep = wall_step / nsubsteps + + fmt = '("' // adjustl(message) // '",' // walltimefmt // ')' + write(*,trim(adjustl(fmt))) wall_main, wall_per_substep + + call self%start() + + return + end subroutine walltime_finish + + module subroutine walltime_reset(self) + !! author: David A. Minton + !! + !! Resets the clock ticker, settting main_start to the current ticker value + use swiftest_globals + implicit none + ! Arguments + class(walltimer), intent(inout) :: self + + call system_clock(self%count_start_main, self%count_rate, self%count_max) + self%lmain_is_started = .true. + call self%start() + + return + end subroutine walltime_reset + + + module subroutine walltime_start(self) + !! author: David A. Minton + !! + !! Starts the timer, setting step_start to the current ticker value + use swiftest_globals + implicit none + ! Arguments + class(walltimer), intent(inout) :: self + + if (.not.self%lmain_is_started) then + write(*,*) "Wall timer error: Cannot start the step time until reset is called at least once!" + return + end if + + call system_clock(self%count_start_step) + + return + end subroutine walltime_start + + +end module walltime_classes \ No newline at end of file diff --git a/src/modules/whm_classes.f90 b/src/modules/whm_classes.f90 index 6d5b26394..9675f289d 100644 --- a/src/modules/whm_classes.f90 +++ b/src/modules/whm_classes.f90 @@ -73,8 +73,8 @@ module whm_classes type, extends(swiftest_nbody_system) :: whm_nbody_system contains !> Replace the abstract procedures with concrete ones - procedure :: initialize => whm_setup_initialize_system !! Performs WHM-specific initilization steps, like calculating the Jacobi masses - procedure :: step => whm_step_system !! Advance the WHM nbody system forward in time by one step + procedure :: initialize => whm_setup_initialize_system ! Performs WHM-specific initilization steps, like calculating the Jacobi masses + procedure :: step => whm_step_system !! Advance the WHM nbody system forward in time by one step end type whm_nbody_system interface @@ -108,6 +108,13 @@ module subroutine whm_drift_pl(self, system, param, dt) real(DP), intent(in) :: dt !! Stepsize end subroutine whm_drift_pl + module subroutine whm_util_index_eucl_plpl(self, param) + use swiftest_classes, only : swiftest_parameters + implicit none + class(whm_pl), intent(inout) :: self !! WHM massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + end subroutine whm_util_index_eucl_plpl + !> Get heliocentric accelration of massive bodies module subroutine whm_kick_getacch_pl(self, system, param, t, lbeg) use swiftest_classes, only : swiftest_cb, swiftest_parameters diff --git a/src/netcdf/netcdf.f90 b/src/netcdf/netcdf.f90 new file mode 100644 index 000000000..80bcdcb5d --- /dev/null +++ b/src/netcdf/netcdf.f90 @@ -0,0 +1,500 @@ +submodule (swiftest_classes) s_netcdf + use swiftest + use netcdf +contains + + subroutine check(status) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Checks the status of all NetCDF operations to catch errors + implicit none + ! Arguments + integer, intent (in) :: status + + if(status /= nf90_noerr) then + write(*,*) trim(nf90_strerror(status)) + call util_exit(FAILURE) + end if + + return + end subroutine check + + module subroutine netcdf_close(self, param) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Closes a NetCDF file + implicit none + ! Arguments + class(netcdf_parameters), intent(inout) :: self !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + + call check( nf90_close(self%ncid) ) + + return + end subroutine netcdf_close + + + module subroutine netcdf_initialize_output(self, param) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Initialize a NetCDF file system and defines all variables. + implicit none + ! Arguments + class(netcdf_parameters), intent(inout) :: self !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + logical :: fileExists + integer(I4B) :: old_mode + + !! Create the new output file, deleting any previously existing output file of the same name + call check( nf90_create(param%outfile, NF90_NETCDF4, self%ncid) ) + call check( nf90_set_fill(self%ncid, nf90_nofill, old_mode) ) + + ! Define the NetCDF dimensions with particle name as the record dimension + call check( nf90_def_dim(self%ncid, ID_DIMNAME, NF90_UNLIMITED, self%id_dimid) ) ! 'x' dimension + call check( nf90_def_dim(self%ncid, TIME_DIMNAME, NF90_UNLIMITED, self%time_dimid) ) ! 'y' dimension + call check( nf90_def_dim(self%ncid, STR_DIMNAME, NAMELEN, self%str_dimid) ) ! Dimension for string variables (aka character arrays) + + select case (param%out_type) + case(NETCDF_FLOAT_TYPE) + self%out_type = NF90_FLOAT + case(NETCDF_DOUBLE_TYPE) + self%out_type = NF90_DOUBLE + end select + + !! Define the variables + call check( nf90_def_var(self%ncid, TIME_DIMNAME, self%out_type, self%time_dimid, self%time_varid) ) + call check( nf90_def_var(self%ncid, ID_DIMNAME, NF90_INT, self%id_dimid, self%id_varid) ) + call check( nf90_def_var(self%ncid, NPL_VARNAME, NF90_INT, self%time_dimid, self%npl_varid) ) + call check( nf90_def_var(self%ncid, NTP_VARNAME, NF90_INT, self%time_dimid, self%ntp_varid) ) + call check( nf90_def_var(self%ncid, NAME_VARNAME, NF90_CHAR, [self%str_dimid, self%id_dimid], self%name_varid) ) + call check( nf90_def_var(self%ncid, PTYPE_VARNAME, NF90_CHAR, [self%str_dimid, self%id_dimid], self%ptype_varid) ) + if ((param%out_form == XV) .or. (param%out_form == XVEL)) then + call check( nf90_def_var(self%ncid, XHX_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%xhx_varid) ) + call check( nf90_def_var(self%ncid, XHY_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%xhy_varid) ) + call check( nf90_def_var(self%ncid, XHZ_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%xhz_varid) ) + call check( nf90_def_var(self%ncid, VHX_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%vhx_varid) ) + call check( nf90_def_var(self%ncid, VHY_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%vhy_varid) ) + call check( nf90_def_var(self%ncid, VHZ_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%vhz_varid) ) + end if + + if ((param%out_form == EL) .or. (param%out_form == XVEL)) then + call check( nf90_def_var(self%ncid, A_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%a_varid) ) + call check( nf90_def_var(self%ncid, E_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%e_varid) ) + call check( nf90_def_var(self%ncid, INC_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%inc_varid) ) + call check( nf90_def_var(self%ncid, CAPOM_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%capom_varid) ) + call check( nf90_def_var(self%ncid, OMEGA_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%omega_varid) ) + call check( nf90_def_var(self%ncid, CAPM_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%capm_varid) ) + end if + + call check( nf90_def_var(self%ncid, GMASS_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%Gmass_varid) ) + if (param%lrhill_present) call check( nf90_def_var(self%ncid, RHILL_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%rhill_varid) ) + if (param%lclose) call check( nf90_def_var(self%ncid, RADIUS_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%radius_varid) ) + if (param%lrotation) then + call check( nf90_def_var(self%ncid, IP1_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%Ip1_varid) ) + call check( nf90_def_var(self%ncid, IP2_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%Ip2_varid) ) + call check( nf90_def_var(self%ncid, IP3_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%Ip3_varid) ) + call check( nf90_def_var(self%ncid, ROTX_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%rotx_varid) ) + call check( nf90_def_var(self%ncid, ROTY_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%roty_varid) ) + call check( nf90_def_var(self%ncid, ROTZ_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%rotz_varid) ) + end if + if (param%ltides) then + call check( nf90_def_var(self%ncid, K2_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%k2_varid) ) + call check( nf90_def_var(self%ncid, Q_VARNAME, self%out_type, [self%id_dimid, self%time_dimid], self%Q_varid) ) + end if + if (param%lenergy) then + call check( nf90_def_var(self%ncid, KE_ORB_VARNAME, self%out_type, self%time_dimid, self%KE_orb_varid) ) + call check( nf90_def_var(self%ncid, KE_SPIN_VARNAME, self%out_type, self%time_dimid, self%KE_spin_varid) ) + call check( nf90_def_var(self%ncid, PE_VARNAME, self%out_type, self%time_dimid, self%PE_varid) ) + call check( nf90_def_var(self%ncid, L_ORBX_VARNAME, self%out_type, self%time_dimid, self%L_orbx_varid) ) + call check( nf90_def_var(self%ncid, L_ORBY_VARNAME, self%out_type, self%time_dimid, self%L_orby_varid) ) + call check( nf90_def_var(self%ncid, L_ORBZ_VARNAME, self%out_type, self%time_dimid, self%L_orbz_varid) ) + call check( nf90_def_var(self%ncid, L_SPINX_VARNAME, self%out_type, self%time_dimid, self%L_spinx_varid) ) + call check( nf90_def_var(self%ncid, L_SPINY_VARNAME, self%out_type, self%time_dimid, self%L_spiny_varid) ) + call check( nf90_def_var(self%ncid, L_SPINZ_VARNAME, self%out_type, self%time_dimid, self%L_spinz_varid) ) + call check( nf90_def_var(self%ncid, L_ESCAPEX_VARNAME, self%out_type, self%time_dimid, self%L_escapex_varid) ) + call check( nf90_def_var(self%ncid, L_ESCAPEY_VARNAME, self%out_type, self%time_dimid, self%L_escapey_varid) ) + call check( nf90_def_var(self%ncid, L_ESCAPEZ_VARNAME, self%out_type, self%time_dimid, self%L_escapez_varid) ) + call check( nf90_def_var(self%ncid, ECOLLISIONS_VARNAME, self%out_type, self%time_dimid, self%Ecollisions_varid) ) + call check( nf90_def_var(self%ncid, EUNTRACKED_VARNAME, self%out_type, self%time_dimid, self%Euntracked_varid) ) + call check( nf90_def_var(self%ncid, GMESCAPE_VARNAME, self%out_type, self%time_dimid, self%GMescape_varid) ) + end if + + call check( nf90_def_var(self%ncid, STATUS_VARNAME, NF90_CHAR, [self%str_dimid, self%id_dimid], self%status_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_TYPE_VARNAME, NF90_CHAR, [self%str_dimid, self%id_dimid], self%origin_type_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_TIME_VARNAME, self%out_type, self%id_dimid, self%origin_time_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_XHX_VARNAME, self%out_type, self%id_dimid, self%origin_xhx_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_XHY_VARNAME, self%out_type, self%id_dimid, self%origin_xhy_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_XHZ_VARNAME, self%out_type, self%id_dimid, self%origin_xhz_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_VHX_VARNAME, self%out_type, self%id_dimid, self%origin_vhx_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_VHY_VARNAME, self%out_type, self%id_dimid, self%origin_vhy_varid) ) + call check( nf90_def_var(self%ncid, ORIGIN_VHZ_VARNAME, self%out_type, self%id_dimid, self%origin_vhz_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_TIME_VARNAME, self%out_type, self%id_dimid, self%discard_time_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_XHX_VARNAME, self%out_type, self%id_dimid, self%discard_xhx_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_XHY_VARNAME, self%out_type, self%id_dimid, self%discard_xhy_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_XHZ_VARNAME, self%out_type, self%id_dimid, self%discard_xhz_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_VHX_VARNAME, self%out_type, self%id_dimid, self%discard_vhx_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_VHY_VARNAME, self%out_type, self%id_dimid, self%discard_vhy_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_VHZ_VARNAME, self%out_type, self%id_dimid, self%discard_vhz_varid) ) + call check( nf90_def_var(self%ncid, DISCARD_BODY_ID_VARNAME, NF90_INT, self%id_dimid, self%discard_body_id_varid) ) + + return + end subroutine netcdf_initialize_output + + + module subroutine netcdf_open(self, param) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Opens a NetCDF file and does the variable inquiries to activate variable ids + implicit none + ! Arguments + class(netcdf_parameters), intent(inout) :: self !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I4B) :: old_mode + + call check( nf90_open(param%outfile, nf90_write, self%ncid) ) + call check( nf90_set_fill(self%ncid, nf90_nofill, old_mode) ) + + call check( nf90_inq_varid(self%ncid, TIME_DIMNAME, self%time_varid)) + call check( nf90_inq_varid(self%ncid, ID_DIMNAME, self%id_varid)) + call check( nf90_inq_varid(self%ncid, NPL_VARNAME, self%npl_varid)) + call check( nf90_inq_varid(self%ncid, NTP_VARNAME, self%ntp_varid)) + call check( nf90_inq_varid(self%ncid, NAME_VARNAME, self%name_varid)) + call check( nf90_inq_varid(self%ncid, PTYPE_VARNAME, self%ptype_varid)) + + if ((param%out_form == XV) .or. (param%out_form == XVEL)) then + call check( nf90_inq_varid(self%ncid, XHX_VARNAME, self%xhx_varid)) + call check( nf90_inq_varid(self%ncid, XHY_VARNAME, self%xhy_varid)) + call check( nf90_inq_varid(self%ncid, XHZ_VARNAME, self%xhz_varid)) + call check( nf90_inq_varid(self%ncid, VHX_VARNAME, self%vhx_varid)) + call check( nf90_inq_varid(self%ncid, VHY_VARNAME, self%vhy_varid)) + call check( nf90_inq_varid(self%ncid, VHZ_VARNAME, self%vhz_varid)) + end if + if ((param%out_form == EL) .or. (param%out_form == XVEL)) then + call check( nf90_inq_varid(self%ncid, A_VARNAME, self%a_varid)) + call check( nf90_inq_varid(self%ncid, E_VARNAME, self%e_varid)) + call check( nf90_inq_varid(self%ncid, INC_VARNAME, self%inc_varid)) + call check( nf90_inq_varid(self%ncid, CAPOM_VARNAME, self%capom_varid)) + call check( nf90_inq_varid(self%ncid, OMEGA_VARNAME, self%omega_varid)) + call check( nf90_inq_varid(self%ncid, CAPM_VARNAME, self%capm_varid)) + end if + call check( nf90_inq_varid(self%ncid, GMASS_VARNAME, self%Gmass_varid)) + if (param%lclose) call check( nf90_inq_varid(self%ncid, RADIUS_VARNAME, self%radius_varid)) + if (param%lrhill_present) call check( nf90_inq_varid(self%ncid, RHILL_VARNAME, self%rhill_varid)) + + if (param%lrotation) then + call check( nf90_inq_varid(self%ncid, IP1_VARNAME, self%Ip1_varid)) + call check( nf90_inq_varid(self%ncid, IP2_VARNAME, self%Ip2_varid)) + call check( nf90_inq_varid(self%ncid, IP3_VARNAME, self%Ip3_varid)) + call check( nf90_inq_varid(self%ncid, ROTX_VARNAME, self%rotx_varid)) + call check( nf90_inq_varid(self%ncid, ROTY_VARNAME, self%roty_varid)) + call check( nf90_inq_varid(self%ncid, ROTZ_VARNAME, self%rotz_varid)) + end if + + if (param%ltides) then + call check( nf90_inq_varid(self%ncid, K2_VARNAME, self%k2_varid)) + call check( nf90_inq_varid(self%ncid, Q_VARNAME, self%Q_varid)) + end if + + if (param%lenergy) then + call check( nf90_inq_varid(self%ncid, KE_ORB_VARNAME, self%KE_orb_varid) ) + call check( nf90_inq_varid(self%ncid, KE_SPIN_VARNAME, self%KE_spin_varid) ) + call check( nf90_inq_varid(self%ncid, PE_VARNAME, self%PE_varid) ) + call check( nf90_inq_varid(self%ncid, L_ORBX_VARNAME, self%L_orbx_varid) ) + call check( nf90_inq_varid(self%ncid, L_ORBY_VARNAME, self%L_orby_varid) ) + call check( nf90_inq_varid(self%ncid, L_ORBZ_VARNAME, self%L_orbz_varid) ) + call check( nf90_inq_varid(self%ncid, L_SPINX_VARNAME, self%L_spinx_varid) ) + call check( nf90_inq_varid(self%ncid, L_SPINY_VARNAME, self%L_spiny_varid) ) + call check( nf90_inq_varid(self%ncid, L_SPINZ_VARNAME, self%L_spinz_varid) ) + call check( nf90_inq_varid(self%ncid, L_ESCAPEX_VARNAME, self%L_escapex_varid) ) + call check( nf90_inq_varid(self%ncid, L_ESCAPEY_VARNAME, self%L_escapey_varid) ) + call check( nf90_inq_varid(self%ncid, L_ESCAPEZ_VARNAME, self%L_escapez_varid) ) + call check( nf90_inq_varid(self%ncid, ECOLLISIONS_VARNAME, self%Ecollisions_varid) ) + call check( nf90_inq_varid(self%ncid, EUNTRACKED_VARNAME, self%Euntracked_varid) ) + call check( nf90_inq_varid(self%ncid, GMESCAPE_VARNAME, self%GMescape_varid) ) + end if + + call check( nf90_inq_varid(self%ncid, STATUS_VARNAME, self%status_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_TYPE_VARNAME, self%origin_type_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_TIME_VARNAME, self%origin_time_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_XHX_VARNAME, self%origin_xhx_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_XHY_VARNAME, self%origin_xhy_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_XHZ_VARNAME, self%origin_xhz_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_VHX_VARNAME, self%origin_vhx_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_VHY_VARNAME, self%origin_vhy_varid)) + call check( nf90_inq_varid(self%ncid, ORIGIN_VHZ_VARNAME, self%origin_vhz_varid)) + + call check( nf90_inq_varid(self%ncid, DISCARD_TIME_VARNAME, self%discard_time_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_XHX_VARNAME, self%discard_xhx_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_XHY_VARNAME, self%discard_xhy_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_XHZ_VARNAME, self%discard_xhz_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_VHX_VARNAME, self%discard_vhx_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_VHY_VARNAME, self%discard_vhy_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_VHZ_VARNAME, self%discard_vhz_varid)) + call check( nf90_inq_varid(self%ncid, DISCARD_BODY_ID_VARNAME, self%discard_body_id_varid)) + + return + end subroutine netcdf_open + + + module subroutine netcdf_write_frame_base(self, iu, param) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Write a frame of output of either test particle or massive body data to the binary output file + !! Note: If outputting to orbital elements, but sure that the conversion is done prior to calling this method + implicit none + ! Arguments + class(swiftest_base), intent(in) :: self !! Swiftest particle object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to identify a particular NetCDF dataset + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I4B) :: i, j, tslot, strlen, idslot + integer(I4B), dimension(:), allocatable :: ind + character(len=:), allocatable :: charstring + + call self%write_particle_info(iu) + + tslot = int(param%ioutput, kind=I4B) + 1 + + select type(self) + class is (swiftest_body) + associate(n => self%nbody) + if (n == 0) return + + allocate(ind(n)) + call util_sort(self%id(1:n), ind) + + do i = 1, n + j = ind(i) + idslot = self%id(j) + 1 + + if ((param%out_form == XV) .or. (param%out_form == XVEL)) then + call check( nf90_put_var(iu%ncid, iu%xhx_varid, self%xh(1, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%xhy_varid, self%xh(2, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%xhz_varid, self%xh(3, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%vhx_varid, self%vh(1, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%vhy_varid, self%vh(2, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%vhz_varid, self%vh(3, j), start=[idslot, tslot]) ) + end if + + if ((param%out_form == EL) .or. (param%out_form == XVEL)) then + call check( nf90_put_var(iu%ncid, iu%a_varid, self%a(j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%e_varid, self%e(j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%inc_varid, self%inc(j) * RAD2DEG, start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%capom_varid, self%capom(j) * RAD2DEG, start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%omega_varid, self%omega(j) * RAD2DEG, start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%capm_varid, self%capm(j) * RAD2DEG, start=[idslot, tslot]) ) + end if + + select type(self) + class is (swiftest_pl) ! Additional output if the passed polymorphic object is a massive body + call check( nf90_put_var(iu%ncid, iu%Gmass_varid, self%Gmass(j), start=[idslot, tslot]) ) + if (param%lrhill_present) then + call check( nf90_put_var(iu%ncid, iu%rhill_varid, self%rhill(j), start=[idslot, tslot]) ) + end if + if (param%lclose) then + call check( nf90_put_var(iu%ncid, iu%radius_varid, self%radius(j), start=[idslot, tslot]) ) + end if + if (param%lrotation) then + call check( nf90_put_var(iu%ncid, iu%Ip1_varid, self%Ip(1, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Ip2_varid, self%Ip(2, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Ip3_varid, self%Ip(3, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%rotx_varid, self%rot(1, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%roty_varid, self%rot(2, j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%rotz_varid, self%rot(3, j), start=[idslot, tslot]) ) + end if + if (param%ltides) then + call check( nf90_put_var(iu%ncid, iu%k2_varid, self%k2(j), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Q_varid, self%Q(j), start=[idslot, tslot]) ) + end if + + end select + end do + end associate + class is (swiftest_cb) + idslot = self%id + 1 + call check( nf90_put_var(iu%ncid, iu%id_varid, self%id, start=[idslot]) ) + + call check( nf90_put_var(iu%ncid, iu%Gmass_varid, self%Gmass, start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%radius_varid, self%radius, start=[idslot, tslot]) ) + if (param%lrotation) then + call check( nf90_put_var(iu%ncid, iu%Ip1_varid, self%Ip(1), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Ip2_varid, self%Ip(2), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Ip3_varid, self%Ip(3), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%rotx_varid, self%rot(1), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%roty_varid, self%rot(2), start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%rotz_varid, self%rot(3), start=[idslot, tslot]) ) + end if + if (param%ltides) then + call check( nf90_put_var(iu%ncid, iu%k2_varid, self%k2, start=[idslot, tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Q_varid, self%Q, start=[idslot, tslot]) ) + end if + + end select + + return + end subroutine netcdf_write_frame_base + + + module subroutine netcdf_write_particle_info_base(self, iu) + !! author: Carlisle A. Wishard, Dana Singh, and David A. Minton + !! + !! Write all current particle to file + implicit none + ! Arguments + class(swiftest_base), intent(in) :: self !! Swiftest particle object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to identify a particular NetCDF dataset + ! Internals + integer(I4B) :: i, j, tslot, strlen, idslot + integer(I4B), dimension(:), allocatable :: ind + character(len=:), allocatable :: charstring + character(len=NAMELEN) :: emptystr, lenstr + character(len=:), allocatable :: fmtlabel + + ! This string of spaces of length NAMELEN is used to clear out any old data left behind inside the string variables + write(lenstr, *) NAMELEN + fmtlabel = "(A" // trim(adjustl(lenstr)) // ")" + write(emptystr, fmtlabel) " " + + select type(self) + class is (swiftest_body) + associate(n => self%nbody) + if (n == 0) return + allocate(ind(n)) + call util_sort(self%id(1:n), ind) + + do i = 1, n + j = ind(i) + idslot = self%id(j) + 1 + call check( nf90_put_var(iu%ncid, iu%id_varid, self%id(j), start=[idslot]) ) + + charstring = trim(adjustl(self%info(j)%name)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%name_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%name_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info(j)%particle_type)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%ptype_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%ptype_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info(j)%status)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%status_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%status_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info(j)%origin_type)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%origin_type_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%origin_type_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + call check( nf90_put_var(iu%ncid, iu%origin_time_varid, self%info(j)%origin_time, start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhx_varid, self%info(j)%origin_xh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhy_varid, self%info(j)%origin_xh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhz_varid, self%info(j)%origin_xh(3), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhx_varid, self%info(j)%origin_vh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhy_varid, self%info(j)%origin_vh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhz_varid, self%info(j)%origin_vh(3), start=[idslot]) ) + + call check( nf90_put_var(iu%ncid, iu%discard_time_varid, self%info(j)%discard_time, start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhx_varid, self%info(j)%discard_xh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhy_varid, self%info(j)%discard_xh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhz_varid, self%info(j)%discard_xh(3), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhx_varid, self%info(j)%discard_vh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhy_varid, self%info(j)%discard_vh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhz_varid, self%info(j)%discard_vh(3), start=[idslot]) ) + end do + end associate + + class is (swiftest_cb) + idslot = self%id + 1 + call check( nf90_put_var(iu%ncid, iu%id_varid, self%id, start=[idslot]) ) + + charstring = trim(adjustl(self%info%name)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%name_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%name_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info%particle_type)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%ptype_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%ptype_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info%status)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%status_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%status_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + charstring = trim(adjustl(self%info%origin_type)) + strlen = len(charstring) + call check( nf90_put_var(iu%ncid, iu%origin_type_varid, emptystr, start=[1, idslot], count=[NAMELEN, 1]) ) + call check( nf90_put_var(iu%ncid, iu%origin_type_varid, charstring, start=[1, idslot], count=[strlen, 1]) ) + + call check( nf90_put_var(iu%ncid, iu%origin_time_varid, self%info%origin_time, start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhx_varid, self%info%origin_xh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhy_varid, self%info%origin_xh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_xhz_varid, self%info%origin_xh(3), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhx_varid, self%info%origin_vh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhy_varid, self%info%origin_vh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%origin_vhz_varid, self%info%origin_vh(3), start=[idslot]) ) + + call check( nf90_put_var(iu%ncid, iu%discard_time_varid, self%info%discard_time, start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhx_varid, self%info%discard_xh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhy_varid, self%info%discard_xh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_xhz_varid, self%info%discard_xh(3), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhx_varid, self%info%discard_vh(1), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhy_varid, self%info%discard_vh(2), start=[idslot]) ) + call check( nf90_put_var(iu%ncid, iu%discard_vhz_varid, self%info%discard_vh(3), start=[idslot]) ) + end select + + return + end subroutine netcdf_write_particle_info_base + + + module subroutine netcdf_write_hdr_system(self, iu, param) + !! author: David A. Minton + !! + !! Writes header information (variables that change with time, but not particle id). + !! This subroutine significantly improves the output over the original binary file, allowing us to track energy, momentum, and other quantities that + !! previously were handled as separate output files. + implicit none + ! Arguments + class(swiftest_nbody_system), intent(in) :: self !! Swiftest nbody system object + class(netcdf_parameters), intent(inout) :: iu !! Parameters used to for writing a NetCDF dataset to file + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I4B) :: tslot, old_mode + + tslot = int(param%ioutput, kind=I4B) + 1 + + call check( nf90_open(param%outfile, nf90_write, iu%ncid) ) + call check( nf90_set_fill(iu%ncid, nf90_nofill, old_mode) ) + + call check( nf90_put_var(iu%ncid, iu%time_varid, param%t, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%npl_varid, self%pl%nbody, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%ntp_varid, self%tp%nbody, start=[tslot]) ) + + if (param%lenergy) then + call check( nf90_put_var(iu%ncid, iu%KE_orb_varid, self%ke_orbit, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%KE_spin_varid, self%ke_spin, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%PE_varid, self%pe, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_orbx_varid, self%Lorbit(1), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_orby_varid, self%Lorbit(2), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_orbz_varid, self%Lorbit(3), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_spinx_varid, self%Lspin(1), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_spiny_varid, self%Lspin(2), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_spinz_varid, self%Lspin(3), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_escapex_varid, param%Lescape(1), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_escapey_varid, param%Lescape(2), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%L_escapez_varid, param%Lescape(3), start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Ecollisions_varid, param%Ecollisions, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%Euntracked_varid, param%Euntracked, start=[tslot]) ) + call check( nf90_put_var(iu%ncid, iu%GMescape_varid, param%GMescape, start=[tslot]) ) + end if + + return + end subroutine netcdf_write_hdr_system + + +end submodule s_netcdf \ No newline at end of file diff --git a/src/obl/obl.f90 b/src/obl/obl.f90 index 035a54b18..977fc620c 100644 --- a/src/obl/obl.f90 +++ b/src/obl/obl.f90 @@ -106,7 +106,8 @@ module subroutine obl_acc_tp(self, system) end subroutine obl_acc_tp - module subroutine obl_pot(npl, Mcb, Mpl, j2rp2, j4rp4, xh, irh, oblpot) + + module subroutine obl_pot_system(self) !! author: David A. Minton !! !! Compute the contribution to the total gravitational potential due solely to the oblateness of the central body @@ -118,33 +119,59 @@ module subroutine obl_pot(npl, Mcb, Mpl, j2rp2, j4rp4, xh, irh, oblpot) !! Adapted from Hal Levison's Swift routine obl_pot.f implicit none ! Arguments - integer(I4B), intent(in) :: npl - real(DP), intent(in) :: Mcb - real(DP), dimension(:), intent(in) :: Mpl - real(DP), intent(in) :: j2rp2, j4rp4 - real(DP), dimension(:), intent(in) :: irh - real(DP), dimension(:, :), intent(in) :: xh - real(DP), intent(out) :: oblpot + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + ! Internals + integer(I4B) :: i + real(DP), dimension(self%pl%nbody) :: oblpot_arr + + associate(system => self, pl => self%pl, npl => self%pl%nbody, cb => self%cb) + if (.not. any(pl%lmask(1:npl))) return + do concurrent (i = 1:npl, pl%lmask(i)) + oblpot_arr(i) = obl_pot_one(npl, cb%Gmass, pl%Gmass(i), cb%j2rp2, cb%j4rp4, pl%xh(3,i), 1.0_DP / norm2(pl%xh(:,i))) + end do + system%oblpot = sum(oblpot_arr, pl%lmask(1:npl)) + end associate + + return + end subroutine obl_pot_system + + + elemental function obl_pot_one(npl, GMcb, GMpl, j2rp2, j4rp4, zh, irh) result(oblpot) + !! author: David A. Minton + !! + !! Compute the contribution to the total gravitational potential due solely to the oblateness of the central body from a single massive body + !! Returned value does not include monopole term or terms higher than J4 + !! + !! Reference: MacMillan, W. D. 1958. The Theory of the Potential, (Dover Publications), 363. + !! + !! Adapted from David E. Kaufmann's Swifter routine: obl_pot.f90 + !! Adapted from Hal Levison's Swift routine obl_pot.f + implicit none + ! Arguments + integer(I4B), intent(in) :: npl !! Number of massive bodies + real(DP), intent(in) :: GMcb !! G*mass of the central body + real(DP), intent(in) :: GMpl !! G*mass of the massive body + real(DP), intent(in) :: j2rp2 !! J_2 / R**2 of the central body + real(DP), intent(in) :: j4rp4 !! J_2 / R**4 of the central body + real(DP), intent(in) :: zh !! z-component of the heliocentric distance vector of the massive body + real(DP), intent(in) :: irh !! Inverse of the heliocentric distance magnitude of the massive body + ! Result + real(DP) :: oblpot !! Gravitational potential ! Internals integer(I4B) :: i real(DP) :: rinv2, t0, t1, t2, t3, p2, p4, mu - oblpot = 0.0_DP - mu = Mcb - do i = 1, npl - rinv2 = irh(i)**2 - t0 = mu * Mpl(i) * rinv2 * irh(i) - t1 = j2rp2 - t2 = xh(3, i) * xh(3, i) * rinv2 - t3 = j4rp4 * rinv2 - p2 = 0.5_DP * (3 * t2 - 1.0_DP) - p4 = 0.125_DP * ((35 * t2 - 30.0_DP) * t2 + 3.0_DP) - oblpot = oblpot + t0 * (t1 * p2 + t3 * p4) - end do + rinv2 = irh**2 + t0 = GMcb * GMpl * rinv2 * irh + t1 = j2rp2 + t2 = zh**2 * rinv2 + t3 = j4rp4 * rinv2 + p2 = 0.5_DP * (3 * t2 - 1.0_DP) + p4 = 0.125_DP * ((35 * t2 - 30.0_DP) * t2 + 3.0_DP) + oblpot = t0 * (t1 * p2 + t3 * p4) return - end subroutine obl_pot - + end function obl_pot_one end submodule s_obl diff --git a/src/orbel/orbel.f90 b/src/orbel/orbel.f90 index f1ab88825..620e0f839 100644 --- a/src/orbel/orbel.f90 +++ b/src/orbel/orbel.f90 @@ -5,7 +5,8 @@ module subroutine orbel_el2xv_vec(self, cb) !! author: David A. Minton !! - !! A wrapper method that converts all of the cartesian position and velocity vectors of a Swiftest body object to orbital elements. + !! A wrapper method that converts all of the orbital element vectors into cartesian position and velocity vectors for a Swiftest body object. + !! This method deallocates all of the orbital elements after it is finished. implicit none ! Arguments class(swiftest_body), intent(inout) :: self !! Swiftest body object @@ -16,10 +17,12 @@ module subroutine orbel_el2xv_vec(self, cb) if (self%nbody == 0) return call self%set_mu(cb) - do i = 1, self%nbody + do concurrent (i = 1:self%nbody) call orbel_el2xv(self%mu(i), self%a(i), self%e(i), self%inc(i), self%capom(i), & self%omega(i), self%capm(i), self%xh(:, i), self%vh(:, i)) end do + deallocate(self%a, self%e, self%inc, self%capom, self%omega, self%capm) + return end subroutine orbel_el2xv_vec @@ -288,7 +291,7 @@ real(DP) pure function orbel_flon(e,icapn) end if return - end function orbel_flon + end function orbel_flon !********************************************************************** @@ -358,7 +361,7 @@ real(DP) pure function orbel_fget(e,capn) !write(*,*) 'fget : returning without complete convergence' return - end function orbel_fget + end function orbel_fget !********************************************************************** @@ -878,19 +881,20 @@ module subroutine orbel_xv2el_vec(self, cb) if (self%nbody == 0) return call self%set_mu(cb) - if (.not.allocated(self%a)) allocate(self%a(self%nbody)) - if (.not.allocated(self%e)) allocate(self%e(self%nbody)) - if (.not.allocated(self%inc)) allocate(self%inc(self%nbody)) - if (.not.allocated(self%capom)) allocate(self%capom(self%nbody)) - if (.not.allocated(self%omega)) allocate(self%omega(self%nbody)) - if (.not.allocated(self%capm)) allocate(self%capm(self%nbody)) - do i = 1, self%nbody + if (allocated(self%a)) deallocate(self%a); allocate(self%a(self%nbody)) + if (allocated(self%e)) deallocate(self%e); allocate(self%e(self%nbody)) + if (allocated(self%inc)) deallocate(self%inc); allocate(self%inc(self%nbody)) + if (allocated(self%capom)) deallocate(self%capom); allocate(self%capom(self%nbody)) + if (allocated(self%omega)) deallocate(self%omega); allocate(self%omega(self%nbody)) + if (allocated(self%capm)) deallocate(self%capm); allocate(self%capm(self%nbody)) + do concurrent (i = 1:self%nbody) call orbel_xv2el(self%mu(i), self%xh(:, i), self%vh(:, i), self%a(i), self%e(i), self%inc(i), & self%capom(i), self%omega(i), self%capm(i)) end do end subroutine orbel_xv2el_vec - pure subroutine orbel_xv2el(mu, x, v, a, e, inc, capom, omega, capm) + + module pure subroutine orbel_xv2el(mu, x, v, a, e, inc, capom, omega, capm) !! author: David A. Minton !! !! Compute osculating orbital elements from relative Cartesian position and velocity @@ -906,9 +910,17 @@ pure subroutine orbel_xv2el(mu, x, v, a, e, inc, capom, omega, capm) !! Adapted from David E. Kaufmann's Swifter routine: orbel_xv2el.f90 !! Adapted from Martin Duncan's Swift routine orbel_xv2el.f implicit none - real(DP), intent(in) :: mu - real(DP), dimension(:), intent(in) :: x, v - real(DP), intent(out) :: a, e, inc, capom, omega, capm + ! Arguments + real(DP), intent(in) :: mu !! Gravitational constant + real(DP), dimension(:), intent(in) :: x !! Position vector + real(DP), dimension(:), intent(in) :: v !! Velocity vector + real(DP), intent(out) :: a !! semimajor axis + real(DP), intent(out) :: e !! eccentricity + real(DP), intent(out) :: inc !! inclination + real(DP), intent(out) :: capom !! longitude of ascending node + real(DP), intent(out) :: omega !! argument of periapsis + real(DP), intent(out) :: capm !! mean anomaly + ! Internals integer(I4B) :: iorbit_type real(DP) :: r, v2, h2, h, rdotv, energy, fac, u, w, cw, sw, face, cape, tmpf, capf real(DP), dimension(NDIM) :: hvec @@ -919,12 +931,12 @@ pure subroutine orbel_xv2el(mu, x, v, a, e, inc, capom, omega, capm) capom = 0.0_DP omega = 0.0_DP capm = 0.0_DP - r = sqrt(dot_product(x(:), x(:))) + r = .mag. x(:) v2 = dot_product(v(:), v(:)) hvec = x(:) .cross. v(:) h2 = dot_product(hvec(:), hvec(:)) - h = sqrt(h2) - if (h2 == 0.0_DP) return + h = .mag. hvec(:) + if (h2 <= 10 * tiny(0.0_DP)) return rdotv = dot_product(x(:), v(:)) energy = 0.5_DP * v2 - mu / r fac = hvec(3) / h diff --git a/src/python_bindings/orbel.f90 b/src/python_bindings/orbel.f90 new file mode 100644 index 000000000..59f24e8b2 --- /dev/null +++ b/src/python_bindings/orbel.f90 @@ -0,0 +1,32 @@ +module orbel + use swiftest + private + public :: xv2el +contains + pure elemental subroutine xv2el(mu, px, py, pz, vx, vy, vz, a, e, inc, capom, omega, capm) + use swiftest_classes, only : orbel_xv2el + implicit none + ! Arguments + real*8, intent(in) :: mu, px, py, pz, vx, vy, vz + real*8, intent(out) :: a, e, inc, capom, omega, capm + !$f2py intent(in) mu + !$f2py intent(in) px + !$f2py intent(in) py + !$f2py intent(in) pz + !$f2py intent(in) vx + !$f2py intent(in) vy + !$f2py intent(in) vz + !$f2py intent(out) a + !$f2py intent(out) e + !$f2py intent(out) inc + !$f2py intent(out) capom + !$f2py intent(out) omega + !$f2py intent(out) capm + ! Internals + real*8, dimension(3) :: x, v + x = [px, py, pz] + v = [vx, vy, vz] + call orbel_xv2el(mu, x(:), v(:), a, e, inc, capom, omega, capm) + return + end subroutine xv2el +end module orbel \ No newline at end of file diff --git a/src/rmvs/rmvs_discard.f90 b/src/rmvs/rmvs_discard.f90 index bcdb9f902..b179178dc 100644 --- a/src/rmvs/rmvs_discard.f90 +++ b/src/rmvs/rmvs_discard.f90 @@ -16,6 +16,7 @@ module subroutine rmvs_discard_tp(self, system, param) class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals integer(I4B) :: i + character(len=STRMAX) :: timestr, idstri, idstrj if (self%nbody == 0) return @@ -25,9 +26,15 @@ module subroutine rmvs_discard_tp(self, system, param) if ((tp%status(i) == ACTIVE) .and. (tp%lperi(i))) then if ((tp%peri(i) < pl%radius(iplperP))) then tp%status(i) = DISCARDED_PLQ - write(*, *) "Particle ",tp%id(i)," q with respect to Planet ",pl%id(iplperP)," is too small at t = ",t + write(idstri, *) tp%id(i) + write(idstrj, *) pl%id(iplperP) + write(timestr, *) t + write(*, *) "Particle " // trim(adjustl(tp%info(i)%name)) // " (" // trim(adjustl(idstri)) & + // ") q with respect to massive body " // trim(adjustl(pl%info(iplperP)%name)) // " (" // trim(adjustl(idstrj)) & + // ") is too small at t = " // trim(adjustl(timestr)) tp%ldiscard(i) = .true. tp%lmask(i) = .false. + call tp%info(i)%set_value(status="DISCARDED_PLQ", discard_time=t, discard_xh=tp%xh(:,i), discard_vh=tp%vh(:,i), discard_body_id=pl%id(iplperP)) end if end if end associate diff --git a/src/rmvs/rmvs_encounter_check.f90 b/src/rmvs/rmvs_encounter_check.f90 index e4c441472..4cb119e48 100644 --- a/src/rmvs/rmvs_encounter_check.f90 +++ b/src/rmvs/rmvs_encounter_check.f90 @@ -23,13 +23,14 @@ module function rmvs_encounter_check_tp(self, system, dt) result(lencounter) real(DP), dimension(system%pl%nbody) :: r2crit logical :: lflag + lencounter = .false. if (self%nbody == 0) return select type(pl => system%pl) class is (rmvs_pl) associate(tp => self, ntp => self%nbody, npl => pl%nbody, rts => system%rts) - r2crit(:) = (rts * pl%rhill(:))**2 - tp%plencP(:) = 0 + r2crit(1:npl) = (rts * pl%rhill(1:npl))**2 + tp%plencP(1:ntp) = 0 do j = 1, npl do i = 1, ntp if ((.not.tp%lmask(i)).or.(tp%plencP(i) /= 0)) cycle @@ -41,9 +42,9 @@ module function rmvs_encounter_check_tp(self, system, dt) result(lencounter) lflag = rmvs_chk_ind(r2, v2, vdotr, dt, r2crit(j)) if (lflag) tp%plencP(i) = j end do - pl%nenc(j) = count(tp%plencP(:) == j) + pl%nenc(j) = count(tp%plencP(1:ntp) == j) end do - lencounter = any(pl%nenc(:) > 0) + lencounter = any(pl%nenc(1:npl) > 0) end associate end select return diff --git a/src/rmvs/rmvs_io.f90 b/src/rmvs/rmvs_io.f90 new file mode 100644 index 000000000..b85ce2202 --- /dev/null +++ b/src/rmvs/rmvs_io.f90 @@ -0,0 +1,48 @@ +submodule (rmvs_classes) s_rmvs_io + use swiftest +contains + + module subroutine rmvs_io_write_encounter(t, id1, id2, Gmass1, Gmass2, radius1, radius2, & + xh1, xh2, vh1, vh2, enc_out) + !! author: David A. Minton + !! + !! Write close encounter data from RMVS to output binary files + !! There is no direct file output from this subroutine + !! + !! Adapted from David E. Kaufmann's Swifter routine: io_write_encounter.f90 + !! Adapted from Hal Levison's Swift routine io_write_encounter.f + implicit none + ! Arguments + integer(I4B), intent(in) :: id1, id2 + real(DP), intent(in) :: t, Gmass1, Gmass2, radius1, radius2 + real(DP), dimension(:), intent(in) :: xh1, xh2, vh1, vh2 + character(*), intent(in) :: enc_out + ! Internals + logical , save :: lfirst = .true. + integer(I4B), parameter :: LUN = 30 + integer(I4B) :: ierr + + if (enc_out == "") return + + open(unit = LUN, file = enc_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) + if ((ierr /= 0) .and. lfirst) then + open(unit = LUN, file = enc_out, status = 'NEW', form = 'UNFORMATTED', iostat = ierr) + end if + if (ierr /= 0) then + write(*, *) "Swiftest Error:" + write(*, *) " Unable to open binary encounter file" + call util_exit(FAILURE) + end if + lfirst = .false. + call io_write_frame_encounter(LUN, t, id1, id2, Gmass1, Gmass2, radius1, radius2, xh1, xh2, vh1, vh2) + close(unit = LUN, iostat = ierr) + if (ierr /= 0) then + write(*, *) "Swiftest Error:" + write(*, *) " Unable to close binary encounter file" + call util_exit(FAILURE) + end if + + return + end subroutine rmvs_io_write_encounter + +end submodule s_rmvs_io \ No newline at end of file diff --git a/src/rmvs/rmvs_kick.f90 b/src/rmvs/rmvs_kick.f90 index 018ada8f3..5d9514763 100644 --- a/src/rmvs/rmvs_kick.f90 +++ b/src/rmvs/rmvs_kick.f90 @@ -61,7 +61,9 @@ module subroutine rmvs_kick_getacch_tp(self, system, param, t, lbeg) end if ! Swap the planetocentric and heliocentric position vectors and central body masses - tp%xh(:,:) = tp%xheliocentric(:,:) + do concurrent(i = 1:ntp, tp%lmask(i)) + tp%xh(:, i) = tp%xheliocentric(:, i) + end do GMcb_original = cb%Gmass cb%Gmass = tp%cb_heliocentric%Gmass @@ -71,7 +73,7 @@ module subroutine rmvs_kick_getacch_tp(self, system, param, t, lbeg) if (param%lgr) call tp%accel_gr(param) ! Put everything back the way we found it - tp%xh(:,:) = xh_original(:,:) + call move_alloc(xh_original, tp%xh) cb%Gmass = GMcb_original end associate diff --git a/src/rmvs/rmvs_setup.f90 b/src/rmvs/rmvs_setup.f90 index 92043e0fe..e59202cd9 100644 --- a/src/rmvs/rmvs_setup.f90 +++ b/src/rmvs/rmvs_setup.f90 @@ -19,7 +19,13 @@ module subroutine rmvs_setup_pl(self, n, param) !> Call allocation method for parent class associate(pl => self) call whm_setup_pl(pl, n, param) - if (n <= 0) return + if (n < 0) return + + if (allocated(pl%outer)) deallocate(pl%outer) + if (allocated(pl%inner)) deallocate(pl%inner) + if (allocated(pl%nenc)) deallocate(pl%nenc) + + if (n == 0) return allocate(pl%outer(0:NTENC)) allocate(pl%inner(0:NTPHENC)) @@ -145,12 +151,14 @@ module subroutine rmvs_setup_tp(self, n, param) !> Call allocation method for parent class. In this case, whm does not have its own setup method, so we use the base method for swiftest_tp call setup_tp(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%lperi)) deallocate(self%lperi) if (allocated(self%plperP)) deallocate(self%plperP) if (allocated(self%plencP)) deallocate(self%plencP) + if (n == 0) return + allocate(self%lperi(n)) allocate(self%plperP(n)) allocate(self%plencP(n)) diff --git a/src/rmvs/rmvs_step.f90 b/src/rmvs/rmvs_step.f90 index 0385aeecc..b8cfcd688 100644 --- a/src/rmvs/rmvs_step.f90 +++ b/src/rmvs/rmvs_step.f90 @@ -21,6 +21,8 @@ module subroutine rmvs_step_system(self, param, t, dt) real(DP), dimension(:,:), allocatable :: xbeg, xend, vbeg integer(I4B) :: i + if (self%tp%nbody == 0) call whm_step_system(self, param, t, dt) + select type(cb => self%cb) class is (rmvs_cb) select type(pl => self%pl) @@ -36,11 +38,11 @@ module subroutine rmvs_step_system(self, param, t, dt) lencounter = tp%encounter_check(system, dt) if (lencounter) then lfirstpl = pl%lfirst - pl%outer(0)%x(:,:) = xbeg(:,:) - pl%outer(0)%v(:,:) = vbeg(:,:) + pl%outer(0)%x(:, 1:npl) = xbeg(:, 1:npl) + pl%outer(0)%v(:, 1:npl) = vbeg(:, 1:npl) call pl%step(system, param, t, dt) - pl%outer(NTENC)%x(:,:) = pl%xh(:,:) - pl%outer(NTENC)%v(:,:) = pl%vh(:,:) + pl%outer(NTENC)%x(:, 1:npl) = pl%xh(:, 1:npl) + pl%outer(NTENC)%v(:, 1:npl) = pl%vh(:, 1:npl) call rmvs_interp_out(cb, pl, dt) call rmvs_step_out(cb, pl, tp, system, param, t, dt) tp%lmask(1:ntp) = .not. tp%lmask(1:ntp) @@ -89,10 +91,10 @@ subroutine rmvs_interp_out(cb, pl, dt) allocate(GMcb(npl)) allocate(dto(npl)) allocate(iflag(npl)) - dto(:) = dt / dntenc - GMcb(:) = cb%Gmass - xtmp(:,:) = pl%outer(0)%x(:, :) - vtmp(:,:) = pl%outer(0)%v(:, :) + dto(1:npl) = dt / dntenc + GMcb(1:npl) = cb%Gmass + xtmp(:,1:npl) = pl%outer(0)%x(:, 1:npl) + vtmp(:,1:npl) = pl%outer(0)%v(:, 1:npl) do outer_index = 1, NTENC - 1 call drift_one(GMcb(1:npl), xtmp(1,1:npl), xtmp(2,1:npl), xtmp(3,1:npl), & vtmp(1,1:npl), vtmp(2,1:npl), vtmp(3,1:npl), & @@ -110,11 +112,11 @@ subroutine rmvs_interp_out(cb, pl, dt) end do end if frac = 1.0_DP - outer_index / dntenc - pl%outer(outer_index)%x(:, :) = frac * xtmp(:,:) - pl%outer(outer_index)%v(:, :) = frac * vtmp(:,:) + pl%outer(outer_index)%x(:, 1:npl) = frac * xtmp(:, 1:npl) + pl%outer(outer_index)%v(:, 1:npl) = frac * vtmp(:, 1:npl) end do - xtmp(:,:) = pl%outer(NTENC)%x(:, :) - vtmp(:,:) = pl%outer(NTENC)%v(:, :) + xtmp(:, 1:npl) = pl%outer(NTENC)%x(:, 1:npl) + vtmp(:, 1:npl) = pl%outer(NTENC)%v(:, 1:npl) do outer_index = NTENC - 1, 1, -1 call drift_one(GMcb(1:npl), xtmp(1,1:npl), xtmp(2,1:npl), xtmp(3,1:npl), & vtmp(1,1:npl), vtmp(2,1:npl), vtmp(3,1:npl), & @@ -132,8 +134,8 @@ subroutine rmvs_interp_out(cb, pl, dt) end do end if frac = outer_index / dntenc - pl%outer(outer_index)%x(:, :) = pl%outer(outer_index)%x(:, :) + frac * xtmp(:,:) - pl%outer(outer_index)%v(:, :) = pl%outer(outer_index)%v(:, :) + frac * vtmp(:,:) + pl%outer(outer_index)%x(:, 1:npl) = pl%outer(outer_index)%x(:, 1:npl) + frac * xtmp(:, 1:npl) + pl%outer(outer_index)%v(:, 1:npl) = pl%outer(outer_index)%v(:, 1:npl) + frac * vtmp(:, 1:npl) end do end associate @@ -165,16 +167,16 @@ subroutine rmvs_step_out(cb, pl, tp, system, param, t, dt) associate(npl => pl%nbody, ntp => tp%nbody) dto = dt / NTENC - where(tp%plencP(:) == 0) - tp%lmask(:) = .false. + where(tp%plencP(1:ntp) == 0) + tp%lmask(1:ntp) = .false. elsewhere - tp%lperi(:) = .false. + tp%lperi(1:ntp) = .false. end where do outer_index = 1, NTENC outer_time = t + (outer_index - 1) * dto - call pl%set_beg_end(xbeg = pl%outer(outer_index - 1)%x(:, :), & - vbeg = pl%outer(outer_index - 1)%v(:, :), & - xend = pl%outer(outer_index )%x(:, :)) + call pl%set_beg_end(xbeg = pl%outer(outer_index - 1)%x(:, 1:npl), & + vbeg = pl%outer(outer_index - 1)%v(:, 1:npl), & + xend = pl%outer(outer_index )%x(:, 1:npl)) system%rts = RHPSCALE lencounter = tp%encounter_check(system, dto) if (lencounter) then @@ -192,8 +194,8 @@ subroutine rmvs_step_out(cb, pl, tp, system, param, t, dt) do j = 1, npl if (pl%nenc(j) == 0) cycle tp%lfirst = .true. - where((tp%plencP(:) == j) .and. (.not.tp%lmask(:))) - tp%lmask(:) = .true. + where((tp%plencP(1:ntp) == j) .and. (.not.tp%lmask(1:ntp))) + tp%lmask(1:ntp) = .true. end where end do end do @@ -222,7 +224,7 @@ subroutine rmvs_interp_in(cb, pl, system, param, dt, outer_index) ! Internals integer(I4B) :: i, inner_index real(DP) :: frac, dntphenc - real(DP), dimension(:,:), allocatable :: xtmp, vtmp, xh_original + real(DP), dimension(:,:), allocatable :: xtmp, vtmp, xh_original, ah_original real(DP), dimension(:), allocatable :: GMcb, dti integer(I4B), dimension(:), allocatable :: iflag @@ -230,32 +232,33 @@ subroutine rmvs_interp_in(cb, pl, system, param, dt, outer_index) dntphenc = real(NTPHENC, kind=DP) ! Set the endpoints of the inner region from the outer region values in the current outer step index - pl%inner(0)%x(:,:) = pl%outer(outer_index - 1)%x(:, :) - pl%inner(0)%v(:,:) = pl%outer(outer_index - 1)%v(:, :) - pl%inner(NTPHENC)%x(:,:) = pl%outer(outer_index)%x(:, :) - pl%inner(NTPHENC)%v(:,:) = pl%outer(outer_index)%v(:, :) + pl%inner(0)%x(:, 1:npl) = pl%outer(outer_index - 1)%x(:, 1:npl) + pl%inner(0)%v(:, 1:npl) = pl%outer(outer_index - 1)%v(:, 1:npl) + pl%inner(NTPHENC)%x(:, 1:npl) = pl%outer(outer_index)%x(:, 1:npl) + pl%inner(NTPHENC)%v(:, 1:npl) = pl%outer(outer_index)%v(:, 1:npl) allocate(xtmp,mold=pl%xh) allocate(vtmp,mold=pl%vh) allocate(GMcb(npl)) allocate(dti(npl)) allocate(iflag(npl)) - dti(:) = dt / dntphenc - GMcb(:) = cb%Gmass - xtmp(:, :) = pl%inner(0)%x(:, :) - vtmp(:, :) = pl%inner(0)%v(:, :) + dti(1:npl) = dt / dntphenc + GMcb(1:npl) = cb%Gmass + xtmp(:, 1:npl) = pl%inner(0)%x(:, 1:npl) + vtmp(:, 1:npl) = pl%inner(0)%v(:, 1:npl) if ((param%loblatecb) .or. (param%ltides)) then allocate(xh_original, source=pl%xh) - pl%xh(:, :) = xtmp(:, :) ! Temporarily replace heliocentric position with inner substep values to calculate the oblateness terms + allocate(ah_original, source=pl%ah) + pl%xh(:, 1:npl) = xtmp(:, 1:npl) ! Temporarily replace heliocentric position with inner substep values to calculate the oblateness terms end if if (param%loblatecb) then call pl%accel_obl(system) - pl%inner(0)%aobl(:, :) = pl%aobl(:, :) ! Save the oblateness acceleration on the planet for this substep + pl%inner(0)%aobl(:, 1:npl) = pl%aobl(:, 1:npl) ! Save the oblateness acceleration on the planet for this substep end if if (param%ltides) then call pl%accel_tides(system) - pl%inner(0)%atide(:, :) = pl%atide(:, :) ! Save the oblateness acceleration on the planet for this substep + pl%inner(0)%atide(:, 1:npl) = pl%atide(:, 1:npl) ! Save the oblateness acceleration on the planet for this substep end if do inner_index = 1, NTPHENC - 1 @@ -275,12 +278,12 @@ subroutine rmvs_interp_in(cb, pl, system, param, dt, outer_index) end do end if frac = 1.0_DP - inner_index / dntphenc - pl%inner(inner_index)%x(:, :) = frac * xtmp(:,:) - pl%inner(inner_index)%v(:, :) = frac * vtmp(:,:) + pl%inner(inner_index)%x(:, 1:npl) = frac * xtmp(:, 1:npl) + pl%inner(inner_index)%v(:, 1:npl) = frac * vtmp(:, 1:npl) end do - xtmp(:,:) = pl%inner(NTPHENC)%x(:, :) - vtmp(:,:) = pl%inner(NTPHENC)%v(:, :) + xtmp(:, 1:npl) = pl%inner(NTPHENC)%x(:, 1:npl) + vtmp(:, 1:npl) = pl%inner(NTPHENC)%v(:, 1:npl) do inner_index = NTPHENC - 1, 1, -1 call drift_one(GMcb(1:npl), xtmp(1,1:npl), xtmp(2,1:npl), xtmp(3,1:npl), & @@ -299,31 +302,32 @@ subroutine rmvs_interp_in(cb, pl, system, param, dt, outer_index) end do end if frac = inner_index / dntphenc - pl%inner(inner_index)%x(:, :) = pl%inner(inner_index)%x(:, :) + frac * xtmp(:, :) - pl%inner(inner_index)%v(:, :) = pl%inner(inner_index)%v(:, :) + frac * vtmp(:, :) + pl%inner(inner_index)%x(:, 1:npl) = pl%inner(inner_index)%x(:, 1:npl) + frac * xtmp(:, 1:npl) + pl%inner(inner_index)%v(:, 1:npl) = pl%inner(inner_index)%v(:, 1:npl) + frac * vtmp(:, 1:npl) if (param%loblatecb) then - pl%xh(:,:) = pl%inner(inner_index)%x(:, :) + pl%xh(:,1:npl) = pl%inner(inner_index)%x(:, 1:npl) call pl%accel_obl(system) - pl%inner(inner_index)%aobl(:, :) = pl%aobl(:, :) + pl%inner(inner_index)%aobl(:, 1:npl) = pl%aobl(:, 1:npl) end if if (param%ltides) then call pl%accel_tides(system) - pl%inner(inner_index)%atide(:, :) = pl%atide(:, :) + pl%inner(inner_index)%atide(:, 1:npl) = pl%atide(:, 1:npl) end if end do if (param%loblatecb) then ! Calculate the final value of oblateness accelerations at the final inner substep - pl%xh(:,:) = pl%inner(NTPHENC)%x(:, :) + pl%xh(:, 1:npl) = pl%inner(NTPHENC)%x(:, 1:npl) call pl%accel_obl(system) - pl%inner(NTPHENC)%aobl(:, :) = pl%aobl(:, :) + pl%inner(NTPHENC)%aobl(:, 1:npl) = pl%aobl(:, 1:npl) end if if (param%ltides) then call pl%accel_tides(system) - pl%inner(NTPHENC)%atide(:, :) = pl%atide(:, :) + pl%inner(NTPHENC)%atide(:, 1:npl) = pl%atide(:, 1:npl) end if - ! Put the planet positions back into place + ! Put the planet positions and accelerations back into place if (allocated(xh_original)) call move_alloc(xh_original, pl%xh) + if (allocated(ah_original)) call move_alloc(ah_original, pl%ah) end associate return @@ -371,7 +375,7 @@ subroutine rmvs_step_in(cb, pl, tp, param, outer_time, dto) ! now step the encountering test particles fully through the inner encounter lfirsttp = .true. do inner_index = 1, NTPHENC ! Integrate over the encounter region, using the "substitute" planetocentric systems at each level - plenci%xh(:,:) = plenci%inner(inner_index - 1)%x(:,:) + plenci%xh(:, 1:npl) = plenci%inner(inner_index - 1)%x(:, 1:npl) call plenci%set_beg_end(xbeg = plenci%inner(inner_index - 1)%x, & xend = plenci%inner(inner_index)%x) @@ -428,7 +432,7 @@ subroutine rmvs_make_planetocentric(param, cb, pl, tp) ! There are inner encounters with this planet if (allocated(encmask)) deallocate(encmask) allocate(encmask(ntp)) - encmask(:) = tp%plencP(:) == i + encmask(1:ntp) = tp%plencP(1:ntp) == i allocate(rmvs_tp :: pl%planetocentric(i)%tp) ! Create encountering test particle structure select type(cbenci => pl%planetocentric(i)%cb) @@ -438,51 +442,53 @@ subroutine rmvs_make_planetocentric(param, cb, pl, tp) select type(tpenci => pl%planetocentric(i)%tp) class is (rmvs_tp) tpenci%lplanetocentric = .true. - call tpenci%setup(pl%nenc(i), param) - tpenci%cb_heliocentric = cb - tpenci%ipleP = i - tpenci%lmask(:) = .true. - tpenci%status(:) = ACTIVE - ! Grab all the encountering test particles and convert them to a planetocentric frame - tpenci%id(:) = pack(tp%id(:), encmask(:)) - do j = 1, NDIM - tpenci%xheliocentric(j, :) = pack(tp%xh(j,:), encmask(:)) - tpenci%xh(j, :) = tpenci%xheliocentric(j, :) - pl%inner(0)%x(j, i) - tpenci%vh(j, :) = pack(tp%vh(j,:), encmask(:)) - pl%inner(0)%v(j, i) - end do - tpenci%lperi(:) = pack(tp%lperi(:), encmask(:)) - tpenci%plperP(:) = pack(tp%plperP(:), encmask(:)) - ! Make sure that the test particles get the planetocentric value of mu - allocate(cbenci%inner(0:NTPHENC)) - do inner_index = 0, NTPHENC - allocate(plenci%inner(inner_index)%x, mold=pl%inner(inner_index)%x) - allocate(plenci%inner(inner_index)%v, mold=pl%inner(inner_index)%x) - allocate(cbenci%inner(inner_index)%x(NDIM,1)) - allocate(cbenci%inner(inner_index)%v(NDIM,1)) - cbenci%inner(inner_index)%x(:,1) = pl%inner(inner_index)%x(:, i) - cbenci%inner(inner_index)%v(:,1) = pl%inner(inner_index)%v(:, i) - plenci%inner(inner_index)%x(:,1) = -cbenci%inner(inner_index)%x(:,1) - plenci%inner(inner_index)%v(:,1) = -cbenci%inner(inner_index)%v(:,1) - - if (param%loblatecb) then - allocate(plenci%inner(inner_index)%aobl, mold=pl%inner(inner_index)%aobl) - allocate(cbenci%inner(inner_index)%aobl(NDIM,1)) - cbenci%inner(inner_index)%aobl(:,1) = pl%inner(inner_index)%aobl(:, i) - end if - - if (param%ltides) then - allocate(plenci%inner(inner_index)%atide, mold=pl%inner(inner_index)%atide) - allocate(cbenci%inner(inner_index)%atide(NDIM,1)) - cbenci%inner(inner_index)%atide(:,1) = pl%inner(inner_index)%atide(:, i) - end if - - do j = 2, npl - ipc2hc = plenci%plind(j) - plenci%inner(inner_index)%x(:,j) = pl%inner(inner_index)%x(:, ipc2hc) - cbenci%inner(inner_index)%x(:,1) - plenci%inner(inner_index)%v(:,j) = pl%inner(inner_index)%v(:, ipc2hc) - cbenci%inner(inner_index)%v(:,1) + associate(nenci => pl%nenc(i)) + call tpenci%setup(nenci, param) + tpenci%cb_heliocentric = cb + tpenci%ipleP = i + tpenci%lmask(1:nenci) = .true. + tpenci%status(1:nenci) = ACTIVE + ! Grab all the encountering test particles and convert them to a planetocentric frame + tpenci%id(1:nenci) = pack(tp%id(1:ntp), encmask(1:ntp)) + do j = 1, NDIM + tpenci%xheliocentric(j, 1:nenci) = pack(tp%xh(j,1:ntp), encmask(:)) + tpenci%xh(j, 1:nenci) = tpenci%xheliocentric(j, 1:nenci) - pl%inner(0)%x(j, i) + tpenci%vh(j, 1:nenci) = pack(tp%vh(j, 1:ntp), encmask(1:ntp)) - pl%inner(0)%v(j, i) + end do + tpenci%lperi(1:nenci) = pack(tp%lperi(1:ntp), encmask(1:ntp)) + tpenci%plperP(1:nenci) = pack(tp%plperP(1:ntp), encmask(1:ntp)) + ! Make sure that the test particles get the planetocentric value of mu + allocate(cbenci%inner(0:NTPHENC)) + do inner_index = 0, NTPHENC + allocate(plenci%inner(inner_index)%x, mold=pl%inner(inner_index)%x) + allocate(plenci%inner(inner_index)%v, mold=pl%inner(inner_index)%x) + allocate(cbenci%inner(inner_index)%x(NDIM,1)) + allocate(cbenci%inner(inner_index)%v(NDIM,1)) + cbenci%inner(inner_index)%x(:,1) = pl%inner(inner_index)%x(:, i) + cbenci%inner(inner_index)%v(:,1) = pl%inner(inner_index)%v(:, i) + plenci%inner(inner_index)%x(:,1) = -cbenci%inner(inner_index)%x(:,1) + plenci%inner(inner_index)%v(:,1) = -cbenci%inner(inner_index)%v(:,1) + + if (param%loblatecb) then + allocate(plenci%inner(inner_index)%aobl, mold=pl%inner(inner_index)%aobl) + allocate(cbenci%inner(inner_index)%aobl(NDIM,1)) + cbenci%inner(inner_index)%aobl(:,1) = pl%inner(inner_index)%aobl(:, i) + end if + + if (param%ltides) then + allocate(plenci%inner(inner_index)%atide, mold=pl%inner(inner_index)%atide) + allocate(cbenci%inner(inner_index)%atide(NDIM,1)) + cbenci%inner(inner_index)%atide(:,1) = pl%inner(inner_index)%atide(:, i) + end if + + do j = 2, npl + ipc2hc = plenci%plind(j) + plenci%inner(inner_index)%x(:,j) = pl%inner(inner_index)%x(:, ipc2hc) - cbenci%inner(inner_index)%x(:,1) + plenci%inner(inner_index)%v(:,j) = pl%inner(inner_index)%v(:, ipc2hc) - cbenci%inner(inner_index)%v(:,1) + end do end do - end do - call tpenci%set_mu(cbenci) + call tpenci%set_mu(cbenci) + end associate end select end select end select @@ -547,8 +553,7 @@ subroutine rmvs_peri_tp(tp, pl, t, dt, lfirst, inner_index, ipleP, param) id2 = tp%id(i) xh2(:) = xpc(:, i) + xh1(:) vh2(:) = xpc(:, i) + vh1(:) - call io_write_encounter(t, id1, id2, mu, 0.0_DP, rpl, 0.0_DP, xh1(:), xh2(:), vh1(:), vh2(:), & - param%enc_out, param%out_type) + call rmvs_io_write_encounter(t, id1, id2, mu, 0.0_DP, rpl, 0.0_DP, xh1(:), xh2(:), vh1(:), vh2(:), param%enc_out) end if if (tp%lperi(i)) then if (peri < tp%peri(i)) then @@ -600,31 +605,33 @@ subroutine rmvs_end_planetocentric(pl, tp) class is (rmvs_pl) select type(tpenci => pl%planetocentric(i)%tp) class is (rmvs_tp) - if (allocated(tpind)) deallocate(tpind) - allocate(tpind(pl%nenc(i))) - ! Index array of encountering test particles - if (allocated(encmask)) deallocate(encmask) - allocate(encmask(ntp)) - encmask(:) = tp%plencP(:) == i - tpind(:) = pack([(j,j=1,ntp)], encmask(:)) - - ! Copy the results of the integration back over and shift back to heliocentric reference - tp%status(tpind(1:pl%nenc(i))) = tpenci%status(1:pl%nenc(i)) - tp%lmask(tpind(1:pl%nenc(i))) = tpenci%lmask(1:pl%nenc(i)) - do j = 1, NDIM - tp%xh(j, tpind(1:pl%nenc(i))) = tpenci%xh(j,1:pl%nenc(i)) + pl%inner(NTPHENC)%x(j, i) - tp%vh(j, tpind(1:pl%nenc(i))) = tpenci%vh(j,1:pl%nenc(i)) + pl%inner(NTPHENC)%v(j, i) - end do - tp%lperi(tpind(1:pl%nenc(i))) = tpenci%lperi(1:pl%nenc(i)) - tp%plperP(tpind(1:pl%nenc(i))) = tpenci%plperP(1:pl%nenc(i)) - deallocate(pl%planetocentric(i)%tp) - deallocate(cbenci%inner) - do inner_index = 0, NTPHENC - deallocate(plenci%inner(inner_index)%x) - deallocate(plenci%inner(inner_index)%v) - if (allocated(plenci%inner(inner_index)%aobl)) deallocate(plenci%inner(inner_index)%aobl) - if (allocated(plenci%inner(inner_index)%atide)) deallocate(plenci%inner(inner_index)%atide) - end do + associate(nenci => pl%nenc(i)) + if (allocated(tpind)) deallocate(tpind) + allocate(tpind(nenci)) + ! Index array of encountering test particles + if (allocated(encmask)) deallocate(encmask) + allocate(encmask(ntp)) + encmask(1:ntp) = tp%plencP(1:ntp) == i + tpind(1:nenci) = pack([(j,j=1,ntp)], encmask(1:ntp)) + + ! Copy the results of the integration back over and shift back to heliocentric reference + tp%status(tpind(1:nenci)) = tpenci%status(1:nenci) + tp%lmask(tpind(1:nenci)) = tpenci%lmask(1:nenci) + do j = 1, NDIM + tp%xh(j, tpind(1:nenci)) = tpenci%xh(j,1:nenci) + pl%inner(NTPHENC)%x(j, i) + tp%vh(j, tpind(1:nenci)) = tpenci%vh(j,1:nenci) + pl%inner(NTPHENC)%v(j, i) + end do + tp%lperi(tpind(1:nenci)) = tpenci%lperi(1:nenci) + tp%plperP(tpind(1:nenci)) = tpenci%plperP(1:nenci) + deallocate(pl%planetocentric(i)%tp) + deallocate(cbenci%inner) + do inner_index = 0, NTPHENC + deallocate(plenci%inner(inner_index)%x) + deallocate(plenci%inner(inner_index)%v) + if (allocated(plenci%inner(inner_index)%aobl)) deallocate(plenci%inner(inner_index)%aobl) + if (allocated(plenci%inner(inner_index)%atide)) deallocate(plenci%inner(inner_index)%atide) + end do + end associate end select end select end select diff --git a/src/rmvs/rmvs_util.f90 b/src/rmvs/rmvs_util.f90 index ee9ce6932..3b823c190 100644 --- a/src/rmvs/rmvs_util.f90 +++ b/src/rmvs/rmvs_util.f90 @@ -189,9 +189,11 @@ module subroutine rmvs_util_sort_pl(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction + if (self%nbody == 0) return + if (ascending) then direction = 1 else @@ -199,6 +201,7 @@ module subroutine rmvs_util_sort_pl(self, sortby, ascending) end if associate(pl => self, npl => self%nbody) + allocate(ind(npl)) select case(sortby) case("nenc") call util_sort(direction * pl%nenc(1:npl), ind(1:npl)) @@ -231,8 +234,10 @@ module subroutine rmvs_util_sort_tp(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind - integer(I4B) :: direction + integer(I4B), dimension(:), allocatable :: ind + integer(I4B) :: direction + + if (self%nbody == 0) return if (ascending) then direction = 1 @@ -241,6 +246,7 @@ module subroutine rmvs_util_sort_tp(self, sortby, ascending) end if associate(tp => self, ntp => self%nbody) + allocate(ind(ntp)) select case(sortby) case("plperP") call util_sort(direction * tp%plperP(1:ntp), ind(1:ntp)) @@ -268,19 +274,14 @@ module subroutine rmvs_util_sort_rearrange_pl(self, ind) ! Arguments class(rmvs_pl), intent(inout) :: self !! RMVS massive body object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - ! Internals - class(rmvs_pl), allocatable :: pl_sorted !! Temporary holder for sorted body - integer(I4B) :: i if (self%nbody == 0) return associate(pl => self, npl => self%nbody) + call util_sort_rearrange(pl%nenc, ind, npl) + call util_sort_rearrange(pl%tpenc1P, ind, npl) + call util_sort_rearrange(pl%plind, ind, npl) call util_sort_rearrange_pl(pl,ind) - allocate(pl_sorted, source=self) - if (allocated(pl%nenc)) pl%nenc(1:npl) = pl_sorted%nenc(ind(1:npl)) - if (allocated(pl%tpenc1P)) pl%tpenc1P(1:npl) = pl_sorted%tpenc1P(ind(1:npl)) - if (allocated(pl%plind)) pl%plind(1:npl) = pl_sorted%plind(ind(1:npl)) - deallocate(pl_sorted) end associate return @@ -296,19 +297,15 @@ module subroutine rmvs_util_sort_rearrange_tp(self, ind) ! Arguments class(rmvs_tp), intent(inout) :: self !! RMVS test particle object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - ! Internals - class(rmvs_tp), allocatable :: tp_sorted !! Temporary holder for sorted body if (self%nbody == 0) return associate(tp => self, ntp => self%nbody) + call util_sort_rearrange(tp%lperi, ind, ntp) + call util_sort_rearrange(tp%plperP, ind, ntp) + call util_sort_rearrange(tp%plencP, ind, ntp) + call util_sort_rearrange(tp%xheliocentric, ind, ntp) call util_sort_rearrange_tp(tp,ind) - allocate(tp_sorted, source=self) - if (allocated(tp%lperi)) tp%lperi(1:ntp) = tp_sorted%lperi(ind(1:ntp)) - if (allocated(tp%plperP)) tp%plperP(1:ntp) = tp_sorted%plperP(ind(1:ntp)) - if (allocated(tp%plencP)) tp%plencP(1:ntp) = tp_sorted%plencP(ind(1:ntp)) - if (allocated(tp%xheliocentric)) tp%xheliocentric(:,1:ntp) = tp_sorted%xheliocentric(:,ind(1:ntp)) - deallocate(tp_sorted) end associate return diff --git a/src/setup/setup.f90 b/src/setup/setup.f90 index 8f96c48a1..41c0d9fba 100644 --- a/src/setup/setup.f90 +++ b/src/setup/setup.f90 @@ -10,7 +10,7 @@ module subroutine setup_construct_system(system, param) implicit none ! Arguments class(swiftest_nbody_system), allocatable, intent(inout) :: system !! Swiftest system object - class(swiftest_parameters), intent(in) :: param !! Swiftest parameters + class(swiftest_parameters), intent(inout) :: param !! Swiftest parameters select case(param%integrator) case (BS) @@ -56,8 +56,9 @@ module subroutine setup_construct_system(system, param) allocate(symba_tp :: system%tp_discards) allocate(symba_merger :: system%pl_adds) allocate(symba_merger :: system%pl_discards) - allocate(symba_plplenc :: system%plplenc_list) allocate(symba_pltpenc :: system%pltpenc_list) + allocate(symba_plplenc :: system%plplenc_list) + allocate(symba_plplenc :: system%plplcollision_list) end select case (RINGMOONS) write(*,*) 'RINGMOONS-SyMBA integrator not yet enabled' @@ -80,40 +81,82 @@ module subroutine setup_encounter(self, n) class(swiftest_encounter), intent(inout) :: self !! Swiftest encounter structure integer(I4B), intent(in) :: n !! Number of encounters to allocate space for - self%nenc = n - if (n == 0) return + if (n < 0) return if (allocated(self%lvdotr)) deallocate(self%lvdotr) if (allocated(self%status)) deallocate(self%status) + if (allocated(self%kidx)) deallocate(self%kidx) if (allocated(self%index1)) deallocate(self%index1) if (allocated(self%index2)) deallocate(self%index2) + if (allocated(self%id1)) deallocate(self%id1) + if (allocated(self%id2)) deallocate(self%id2) if (allocated(self%x1)) deallocate(self%x1) if (allocated(self%x2)) deallocate(self%x2) if (allocated(self%v1)) deallocate(self%v1) if (allocated(self%v2)) deallocate(self%v2) + if (allocated(self%t)) deallocate(self%t) + + self%nenc = n + if (n == 0) return allocate(self%lvdotr(n)) allocate(self%status(n)) + allocate(self%kidx(n)) allocate(self%index1(n)) allocate(self%index2(n)) + allocate(self%id1(n)) + allocate(self%id2(n)) allocate(self%x1(NDIM,n)) allocate(self%x2(NDIM,n)) allocate(self%v1(NDIM,n)) allocate(self%v2(NDIM,n)) + allocate(self%t(n)) self%lvdotr(:) = .false. self%status(:) = INACTIVE + self%kidx(:) = 0_I8B self%index1(:) = 0 self%index2(:) = 0 + self%id1(:) = 0 + self%id2(:) = 0 self%x1(:,:) = 0.0_DP self%x2(:,:) = 0.0_DP self%v1(:,:) = 0.0_DP self%v2(:,:) = 0.0_DP + self%t(:) = 0.0_DP return end subroutine setup_encounter + module subroutine setup_initialize_particle_info_system(self, param) + !! author: David A. Minton + !! + !! Setup up particle information metadata from initial conditions + ! + implicit none + ! Arguments + class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters + ! Internals + integer(I4B) :: i + + associate(cb => self%cb, pl => self%pl, npl => self%pl%nbody, tp => self%tp, ntp => self%tp%nbody) + + call cb%info%set_value(particle_type=CB_TYPE_NAME, status="ACTIVE", origin_type="Initial conditions", origin_time=param%t0, origin_xh=[0.0_DP, 0.0_DP, 0.0_DP], origin_vh=[0.0_DP, 0.0_DP, 0.0_DP]) + do i = 1, self%pl%nbody + call pl%info(i)%set_value(particle_type=PL_TYPE_NAME, status="ACTIVE", origin_type="Initial conditions", origin_time=param%t0, origin_xh=self%pl%xh(:,i), origin_vh=self%pl%vh(:,i)) + end do + do i = 1, self%tp%nbody + call tp%info(i)%set_value(particle_type=TP_TYPE_NAME, status="ACTIVE", origin_type="Initial conditions", origin_time=param%t0, origin_xh=self%tp%xh(:,i), origin_vh=self%tp%vh(:,i)) + end do + + end associate + + return + end subroutine setup_initialize_particle_info_system + + module subroutine setup_initialize_system(self, param) !! author: David A. Minton !! @@ -123,16 +166,28 @@ module subroutine setup_initialize_system(self, param) ! Arguments class(swiftest_nbody_system), intent(inout) :: self !! Swiftest system object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - - call self%cb%initialize(param) - call self%pl%initialize(param) - call self%tp%initialize(param) + + call self%cb%read_in(param) + call self%pl%read_in(param) + call self%tp%read_in(param) call self%validate_ids(param) call self%set_msys() call self%pl%set_mu(self%cb) call self%tp%set_mu(self%cb) - call self%pl%eucl_index() + if (param%in_form == EL) then + call self%pl%el2xv(self%cb) + call self%tp%el2xv(self%cb) + end if + call self%pl%index(param) if (.not.param%lrhill_present) call self%pl%set_rhill(self%cb) + self%pl%lfirst = param%lfirstkick + self%tp%lfirst = param%lfirstkick + + if (param%lrestart) then + call self%read_particle_info(param) + else + call self%init_particle_info(param) + end if return end subroutine setup_initialize_system @@ -148,39 +203,69 @@ module subroutine setup_body(self, n, param) class(swiftest_body), intent(inout) :: self !! Swiftest generic body object integer(I4B), intent(in) :: n !! Number of particles to allocate space for class(swiftest_parameters), intent(in) :: param !! Current run configuration parameter + ! Internals + integer(I4B) :: i + + if (n < 0) return - self%nbody = n - if (n <= 0) return self%lfirst = .true. + if (allocated(self%info)) deallocate(self%info) if (allocated(self%id)) deallocate(self%id) - if (allocated(self%name)) deallocate(self%name) if (allocated(self%status)) deallocate(self%status) if (allocated(self%ldiscard)) deallocate(self%ldiscard) + if (allocated(self%lmask)) deallocate(self%lmask) + if (allocated(self%mu)) deallocate(self%mu) if (allocated(self%xh)) deallocate(self%xh) if (allocated(self%vh)) deallocate(self%vh) if (allocated(self%xb)) deallocate(self%xb) if (allocated(self%vb)) deallocate(self%vb) if (allocated(self%ah)) deallocate(self%ah) + if (allocated(self%aobl)) deallocate(self%aobl) + if (allocated(self%agr)) deallocate(self%lmask) + if (allocated(self%atide)) deallocate(self%lmask) if (allocated(self%ir3h)) deallocate(self%ir3h) - if (allocated(self%mu)) deallocate(self%mu) - if (allocated(self%lmask)) deallocate(self%lmask) + if (allocated(self%a)) deallocate(self%a) + if (allocated(self%e)) deallocate(self%e) + if (allocated(self%e)) deallocate(self%e) + if (allocated(self%inc)) deallocate(self%inc) + if (allocated(self%capom)) deallocate(self%capom) + if (allocated(self%omega)) deallocate(self%omega) + if (allocated(self%capm)) deallocate(self%capm) + + self%nbody = n + if (n == 0) return + allocate(self%info(n)) allocate(self%id(n)) - allocate(self%name(n)) allocate(self%status(n)) allocate(self%ldiscard(n)) + allocate(self%lmask(n)) + allocate(self%mu(n)) allocate(self%xh(NDIM, n)) allocate(self%vh(NDIM, n)) allocate(self%xb(NDIM, n)) allocate(self%vb(NDIM, n)) allocate(self%ah(NDIM, n)) allocate(self%ir3h(n)) - allocate(self%mu(n)) - allocate(self%lmask(n)) - self%id(:) = 0 - self%name(:) = "UNNAMED" + self%id(:) = 0 + do i = 1, n + call self%info(i)%set_value(& + name = "UNNAMED", & + particle_type = "UNKNOWN", & + status = "INACTIVE", & + origin_type = "UNKNOWN", & + origin_time = -huge(1.0_DP), & + origin_xh = [0.0_DP, 0.0_DP, 0.0_DP], & + origin_vh = [0.0_DP, 0.0_DP, 0.0_DP], & + discard_time = -huge(1.0_DP), & + discard_xh = [0.0_DP, 0.0_DP, 0.0_DP], & + discard_vh = [0.0_DP, 0.0_DP, 0.0_DP], & + discard_body_id = -1 & + ) + end do + self%status(:) = INACTIVE self%lmask(:) = .false. self%ldiscard(:) = .false. @@ -193,17 +278,14 @@ module subroutine setup_body(self, n, param) self%mu(:) = 0.0_DP if (param%loblatecb) then - if (allocated(self%aobl)) deallocate(self%aobl) allocate(self%aobl(NDIM, n)) self%aobl(:,:) = 0.0_DP end if if (param%ltides) then - if (allocated(self%atide)) deallocate(self%lmask) allocate(self%atide(NDIM, n)) self%atide(:,:) = 0.0_DP end if if (param%lgr) then - if (allocated(self%agr)) deallocate(self%lmask) allocate(self%agr(NDIM, n)) self%agr(:,:) = 0.0_DP end if @@ -226,11 +308,20 @@ module subroutine setup_pl(self, n, param) !> Call allocation method for parent class !> The parent class here is the abstract swiftest_body class, so we can't use the type-bound procedure call setup_body(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%mass)) deallocate(self%mass) if (allocated(self%Gmass)) deallocate(self%Gmass) if (allocated(self%rhill)) deallocate(self%rhill) + if (allocated(self%radius)) deallocate(self%radius) + if (allocated(self%density)) deallocate(self%density) + if (allocated(self%rot)) deallocate(self%rot) + if (allocated(self%Ip)) deallocate(self%Ip) + if (allocated(self%k2)) deallocate(self%k2) + if (allocated(self%Q)) deallocate(self%Q) + if (allocated(self%tlag)) deallocate(self%tlag) + + if (n == 0) return allocate(self%mass(n)) allocate(self%Gmass(n)) @@ -243,8 +334,6 @@ module subroutine setup_pl(self, n, param) self%nplpl = 0 if (param%lclose) then - if (allocated(self%radius)) deallocate(self%radius) - if (allocated(self%density)) deallocate(self%density) allocate(self%radius(n)) allocate(self%density(n)) self%radius(:) = 0.0_DP @@ -252,8 +341,6 @@ module subroutine setup_pl(self, n, param) end if if (param%lrotation) then - if (allocated(self%rot)) deallocate(self%rhill) - if (allocated(self%Ip)) deallocate(self%rhill) allocate(self%rot(NDIM, n)) allocate(self%Ip(NDIM, n)) self%rot(:,:) = 0.0_DP @@ -261,9 +348,6 @@ module subroutine setup_pl(self, n, param) end if if (param%ltides) then - if (allocated(self%k2)) deallocate(self%rhill) - if (allocated(self%Q)) deallocate(self%rhill) - if (allocated(self%tlag)) deallocate(self%rhill) allocate(self%k2(n)) allocate(self%Q(n)) allocate(self%tlag(n)) @@ -290,12 +374,14 @@ module subroutine setup_tp(self, n, param) !> Call allocation method for parent class !> The parent class here is the abstract swiftest_body class, so we can't use the type-bound procedure call setup_body(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%isperi)) deallocate(self%isperi) if (allocated(self%peri)) deallocate(self%peri) if (allocated(self%atp)) deallocate(self%atp) + if (n == 0) return + allocate(self%isperi(n)) allocate(self%peri(n)) allocate(self%atp(n)) diff --git a/src/symba/symba_collision.f90 b/src/symba/symba_collision.f90 index 1910411b9..a3990cabd 100644 --- a/src/symba/symba_collision.f90 +++ b/src/symba/symba_collision.f90 @@ -1,8 +1,256 @@ submodule (symba_classes) s_symba_collision use swiftest + contains - module subroutine symba_collision_check_pltpenc(self, system, param, t, dt, irec) + module function symba_collision_casedisruption(system, param, colliders, frag) result(status) + !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Create the fragments resulting from a non-catastrophic disruption collision + !! + implicit none + ! Arguments + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + ! Result + integer(I4B) :: status !! Status flag assigned to this outcome + ! Internals + integer(I4B) :: i, nfrag + logical :: lfailure + character(len=STRMAX) :: message + + select case(frag%regime) + case(COLLRESOLVE_REGIME_DISRUPTION) + message = "Disruption between" + case(COLLRESOLVE_REGIME_SUPERCATASTROPHIC) + message = "Supercatastrophic disruption between" + end select + call symba_collision_collider_message(system%pl, colliders%idx, message) + call fraggle_io_log_one_message(message) + + ! Collisional fragments will be uniformly distributed around the pre-impact barycenter + call frag%set_mass_dist(colliders, param) + + ! Generate the position and velocity distributions of the fragments + call frag%generate_fragments(colliders, system, param, lfailure) + + if (lfailure) then + call fraggle_io_log_one_message("No fragment solution found, so treat as a pure hit-and-run") + status = ACTIVE + nfrag = 0 + select type(pl => system%pl) + class is (symba_pl) + pl%status(colliders%idx(:)) = status + pl%ldiscard(colliders%idx(:)) = .false. + pl%lcollision(colliders%idx(:)) = .false. + end select + else + ! Populate the list of new bodies + nfrag = frag%nbody + write(message, *) nfrag + call fraggle_io_log_one_message("Generating " // trim(adjustl(message)) // " fragments") + select case(frag%regime) + case(COLLRESOLVE_REGIME_DISRUPTION) + status = DISRUPTION + case(COLLRESOLVE_REGIME_SUPERCATASTROPHIC) + status = SUPERCATASTROPHIC + end select + frag%id(1:nfrag) = [(i, i = param%maxid + 1, param%maxid + nfrag)] + param%maxid = frag%id(nfrag) + call symba_collision_mergeaddsub(system, param, colliders, frag, status) + end if + + return + end function symba_collision_casedisruption + + + module function symba_collision_casehitandrun(system, param, colliders, frag) result(status) + !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Create the fragments resulting from a non-catastrophic hit-and-run collision + !! + implicit none + ! Arguments + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + ! Result + integer(I4B) :: status !! Status flag assigned to this outcom + ! Internals + integer(I4B) :: i, ibiggest, nfrag, jtarg, jproj + logical :: lpure + character(len=STRMAX) :: message + character(len=NAMELEN) :: idstr + + message = "Hit and run between" + call symba_collision_collider_message(system%pl, colliders%idx, message) + call fraggle_io_log_one_message(trim(adjustl(message))) + + if (colliders%mass(1) > colliders%mass(2)) then + jtarg = 1 + jproj = 2 + else + jtarg = 2 + jproj = 1 + end if + + if (frag%mass_dist(2) > 0.9_DP * colliders%mass(jproj)) then ! Pure hit and run, so we'll just keep the two bodies untouched + call fraggle_io_log_one_message("Pure hit and run. No new fragments generated.") + nfrag = 0 + lpure = .true. + else ! Imperfect hit and run, so we'll keep the largest body and destroy the other + lpure = .false. + call frag%set_mass_dist(colliders, param) + + ! Generate the position and velocity distributions of the fragments + call frag%generate_fragments(colliders, system, param, lpure) + + if (lpure) then + call fraggle_io_log_one_message("Should have been a pure hit and run instead") + nfrag = 0 + else + nfrag = frag%nbody + write(message, *) nfrag + call fraggle_io_log_one_message("Generating " // trim(adjustl(message)) // " fragments") + end if + end if + if (lpure) then ! Reset these bodies back to being active so that nothing further is done to them + status = HIT_AND_RUN_PURE + select type(pl => system%pl) + class is (symba_pl) + pl%status(colliders%idx(:)) = ACTIVE + pl%ldiscard(colliders%idx(:)) = .false. + pl%lcollision(colliders%idx(:)) = .false. + end select + else + ibiggest = colliders%idx(maxloc(system%pl%Gmass(colliders%idx(:)), dim=1)) + frag%id(1) = system%pl%id(ibiggest) + frag%id(2:nfrag) = [(i, i = param%maxid + 1, param%maxid + nfrag - 1)] + param%maxid = frag%id(nfrag) + status = HIT_AND_RUN_DISRUPT + call symba_collision_mergeaddsub(system, param, colliders, frag, status) + end if + + return + end function symba_collision_casehitandrun + + + module function symba_collision_casemerge(system, param, colliders, frag) result(status) + !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton + !! + !! Merge massive bodies. + !! + !! Adapted from David E. Kaufmann's Swifter routines symba_merge_pl.f90 and symba_discard_merge_pl.f90 + !! + !! Adapted from Hal Levison's Swift routines symba5_merge.f and discard_mass_merge.f + implicit none + ! Arguments + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + ! Result + integer(I4B) :: status !! Status flag assigned to this outcome + ! Internals + integer(I4B) :: i, j, k, ibiggest + real(DP), dimension(2) :: volume, density + real(DP) :: pe + real(DP), dimension(NDIM) :: L_spin_new + character(len=NAMELEN) :: idstr + character(len=STRMAX) :: message + + message = "Merging" + call symba_collision_collider_message(system%pl, colliders%idx, message) + call fraggle_io_log_one_message(message) + + select type(pl => system%pl) + class is (symba_pl) + + call frag%set_mass_dist(colliders, param) + ibiggest = colliders%idx(maxloc(pl%Gmass(colliders%idx(:)), dim=1)) + frag%id(1) = pl%id(ibiggest) + frag%xb(:,1) = frag%xbcom(:) + frag%vb(:,1) = frag%vbcom(:) + + if (param%lrotation) then + ! Conserve angular momentum by putting pre-impact orbital momentum into spin of the new body + L_spin_new(:) = colliders%L_orbit(:,1) + colliders%L_orbit(:,2) + colliders%L_spin(:,1) + colliders%L_spin(:,2) + + ! Assume prinicpal axis rotation on 3rd Ip axis + frag%rot(:,1) = L_spin_new(:) / (frag%Ip(3,1) * frag%mass(1) * frag%radius(1)**2) + else ! If spin is not enabled, we will consider the lost pre-collision angular momentum as "escaped" and add it to our bookkeeping variable + param%Lescape(:) = param%Lescape(:) + colliders%L_orbit(:,1) + colliders%L_orbit(:,2) + end if + + ! Keep track of the component of potential energy due to the pre-impact colliders%idx for book-keeping + pe = 0.0_DP + do j = 1, colliders%ncoll + do i = j + 1, colliders%ncoll + pe = pe - pl%Gmass(i) * pl%mass(j) / norm2(pl%xb(:, i) - pl%xb(:, j)) + end do + end do + param%Ecollisions = param%Ecollisions + pe + param%Euntracked = param%Euntracked - pe + + ! Update any encounter lists that have the removed bodies in them so that they instead point to the new + do k = 1, system%plplenc_list%nenc + do j = 1, colliders%ncoll + i = colliders%idx(j) + if (i == ibiggest) cycle + if (system%plplenc_list%id1(k) == pl%id(i)) then + system%plplenc_list%id1(k) = pl%id(ibiggest) + system%plplenc_list%index1(k) = i + end if + if (system%plplenc_list%id2(k) == pl%id(i)) then + system%plplenc_list%id2(k) = pl%id(ibiggest) + system%plplenc_list%index2(k) = i + end if + if (system%plplenc_list%id1(k) == system%plplenc_list%id2(k)) system%plplenc_list%status(k) = INACTIVE + end do + end do + + status = MERGED + + call symba_collision_mergeaddsub(system, param, colliders, frag, status) + + end select + + return + end function symba_collision_casemerge + + + subroutine symba_collision_collider_message(pl, collidx, collider_message) + !! author: David A. Minton + !! + !! Prints a nicely formatted message about which bodies collided, including their names and ids. + !! This subroutine appends the body names and ids to an input message. + implicit none + ! Arguments + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object + integer(I4B), dimension(:), intent(in) :: collidx !! Index of collisional colliders%idx members + character(*), intent(inout) :: collider_message !! The message to print to the screen. + ! Internals + integer(I4B) :: i, n + character(len=STRMAX) :: idstr + + n = size(collidx) + if (n == 0) return + + do i = 1, n + if (i > 1) collider_message = trim(adjustl(collider_message)) // " and " + collider_message = " " // trim(adjustl(collider_message)) // " " // trim(adjustl(pl%info(collidx(i))%name)) + write(idstr, '(I10)') pl%id(collidx(i)) + collider_message = trim(adjustl(collider_message)) // " (" // trim(adjustl(idstr)) // ") " + end do + + return + end subroutine symba_collision_collider_message + + + module function symba_collision_check_encounter(self, system, param, t, dt, irec) result(lany_collision) !! author: David A. Minton !! !! Check for merger between massive bodies and test particles in SyMBA @@ -12,20 +260,26 @@ module subroutine symba_collision_check_pltpenc(self, system, param, t, dt, irec !! Adapted from Hal Levison's Swift routine symba5_merge.f implicit none ! Arguments - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter list object - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters - real(DP), intent(in) :: t !! current time - real(DP), intent(in) :: dt !! step size - integer(I4B), intent(in) :: irec !! Current recursion level + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter list object + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + real(DP), intent(in) :: t !! current time + real(DP), intent(in) :: dt !! step size + integer(I4B), intent(in) :: irec !! Current recursion level + ! Result + logical :: lany_collision !! Returns true if cany pair of encounters resulted in a collision ! Internals logical, dimension(:), allocatable :: lcollision, lmask real(DP), dimension(NDIM) :: xr, vr - integer(I4B) :: k + integer(I4B) :: i, j, k, nenc real(DP) :: rlim, Gmtot logical :: isplpl + character(len=STRMAX) :: timestr, idstri, idstrj, message + + lany_collision = .false. if (self%nenc == 0) return + select type(self) class is (symba_plplenc) isplpl = .true. @@ -37,67 +291,93 @@ module subroutine symba_collision_check_pltpenc(self, system, param, t, dt, irec class is (symba_pl) select type(tp => system%tp) class is (symba_tp) - associate(nenc => self%nenc, ind1 => self%index1, ind2 => self%index2) - allocate(lmask(nenc)) - lmask(:) = ((self%status(1:nenc) == ACTIVE) .and. (pl%levelg(ind1(1:nenc)) >= irec)) - if (isplpl) then - lmask(:) = lmask(:) .and. (pl%levelg(ind2(1:nenc)) >= irec) - else - lmask(:) = lmask(:) .and. (tp%levelg(ind2(1:nenc)) >= irec) - end if - if (.not.any(lmask(:))) return + nenc = self%nenc + nenc = self%nenc + allocate(lmask(nenc)) + lmask(:) = ((self%status(1:nenc) == ACTIVE) .and. (pl%levelg(self%index1(1:nenc)) >= irec)) + if (isplpl) then + lmask(:) = lmask(:) .and. (pl%levelg(self%index2(1:nenc)) >= irec) + else + lmask(:) = lmask(:) .and. (tp%levelg(self%index2(1:nenc)) >= irec) + end if + if (.not.any(lmask(:))) return - allocate(lcollision(nenc)) - lcollision(:) = .false. + allocate(lcollision(nenc)) + lcollision(:) = .false. + if (isplpl) then + do concurrent(k = 1:nenc, lmask(k)) + i = self%index1(k) + j = self%index2(k) + xr(:) = pl%xh(:, i) - pl%xh(:, j) + vr(:) = pl%vb(:, i) - pl%vb(:, j) + rlim = pl%radius(i) + pl%radius(j) + Gmtot = pl%Gmass(i) + pl%Gmass(j) + lcollision(k) = symba_collision_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), Gmtot, rlim, dt, self%lvdotr(k)) + end do + else + do concurrent(k = 1:nenc, lmask(k)) + i = self%index1(k) + j = self%index2(k) + xr(:) = pl%xh(:, i) - tp%xh(:, j) + vr(:) = pl%vb(:, i) - tp%vb(:, j) + lcollision(k) = symba_collision_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%Gmass(i), pl%radius(i), dt, self%lvdotr(k)) + end do + end if + + if (any(lcollision(1:nenc))) call pl%xh2xb(system%cb) ! Update the central body barycenteric position vector to get us out of DH and into bary + do k = 1, nenc + i = self%index1(k) + j = self%index2(k) + if (lcollision(k)) self%status(k) = COLLISION + self%t(k) = t + self%x1(:,k) = pl%xh(:,i) + system%cb%xb(:) + self%v1(:,k) = pl%vb(:,i) if (isplpl) then - do concurrent(k = 1:nenc, lmask(k)) - xr(:) = pl%xh(:, ind1(k)) - pl%xh(:, ind2(k)) - vr(:) = pl%vb(:, ind1(k)) - pl%vb(:, ind2(k)) - rlim = pl%radius(ind1(k)) + pl%radius(ind2(k)) - Gmtot = pl%Gmass(ind1(k)) + pl%Gmass(ind2(k)) - lcollision(k) = symba_collision_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), Gmtot, rlim, dt, self%lvdotr(k)) - end do - else - do concurrent(k = 1:nenc, lmask(k)) - xr(:) = pl%xh(:, ind1(k)) - tp%xh(:, ind2(k)) - vr(:) = pl%vb(:, ind1(k)) - tp%vb(:, ind2(k)) - lcollision(k) = symba_collision_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%Gmass(ind1(k)), pl%radius(ind1(k)), dt, self%lvdotr(k)) - end do - end if + self%x2(:,k) = pl%xh(:,j) + system%cb%xb(:) + self%v2(:,k) = pl%vb(:,j) + if (lcollision(k)) then + ! Check to see if either of these bodies has been involved with a collision before, and if so, make this a collisional colliders%idx + if (pl%lcollision(i) .or. pl%lcollision(j)) call pl%make_colliders([i,j]) - if (any(lcollision(:))) then - do k = 1, nenc - if (.not.lcollision(k)) cycle - self%status(k) = COLLISION - self%x1(:,k) = pl%xh(:,ind1(k)) - self%v1(:,k) = pl%vb(:,ind1(k)) - if (isplpl) then - self%x2(:,k) = pl%xh(:,ind2(k)) - self%v2(:,k) = pl%vb(:,ind2(k)) - - ! Check to see if either of these bodies has been involved with a collision before, and if so, make this a collisional family - if (pl%lcollision(ind1(k)) .or. pl%lcollision(ind2(k))) call pl%make_family([ind1(k),ind2(k)]) - - ! Set the collision flag for these to bodies to true in case they become involved in another collision later in the step - pl%lcollision([ind1(k), ind2(k)]) = .true. - pl%ldiscard([ind1(k), ind2(k)]) = .true. - pl%status([ind1(k), ind2(k)]) = COLLISION - else - self%x2(:,k) = tp%xh(:,ind2(k)) - self%v2(:,k) = tp%vb(:,ind2(k)) - tp%status(ind2(k)) = DISCARDED_PLR - tp%ldiscard(ind2(k)) = .true. - write(*,*) 'Test particle ',tp%id(ind2(k)), ' collided with massive body ',pl%id(ind1(k)), ' at time ',t - end if - end do + ! Set the collision flag for these to bodies to true in case they become involved in another collision later in the step + pl%lcollision([i, j]) = .true. + pl%status([i, j]) = COLLISION + call pl%info(i)%set_value(status="COLLISION", discard_time=t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i)) + call pl%info(j)%set_value(status="COLLISION", discard_time=t, discard_xh=pl%xh(:,j), discard_vh=pl%vh(:,j)) + end if + else + self%x2(:,k) = tp%xh(:,j) + system%cb%xb(:) + self%v2(:,k) = tp%vb(:,j) + if (lcollision(k)) then + tp%status(j) = DISCARDED_PLR + tp%ldiscard(j) = .true. + write(idstri, *) pl%id(i) + write(idstrj, *) tp%id(j) + write(timestr, *) t + call tp%info(j)%set_value(status="DISCARDED_PLR", discard_time=t, discard_xh=tp%xh(:,j), discard_vh=tp%vh(:,j)) + write(message, *) "Particle " // trim(adjustl(tp%info(j)%name)) // " (" // trim(adjustl(idstrj)) // ")" & + // " collided with massive body " // trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstri)) // ")" & + // " at t = " // trim(adjustl(timestr)) + call fraggle_io_log_one_message(message) + end if end if - end associate + end do end select end select + lany_collision = any(lcollision(:)) + + ! Extract the pl-pl encounter list and return the plplcollision_list + if (lany_collision) then + select type(plplenc_list => self) + class is (symba_plplenc) + call plplenc_list%extract_collisions(system, param) + end select + end if + return - end subroutine symba_collision_check_pltpenc + end function symba_collision_check_encounter pure elemental function symba_collision_check_one(xr, yr, zr, vxr, vyr, vzr, Gmtot, rlim, dt, lvdotr) result(lcollision) @@ -143,32 +423,32 @@ pure elemental function symba_collision_check_one(xr, yr, zr, vxr, vyr, vzr, Gmt end function symba_collision_check_one - function symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v, mass, radius, L_spin, Ip) result(lflag) + function symba_collision_consolidate_colliders(pl, cb, param, idx_parent, colliders) result(lflag) !! author: David A. Minton !! - !! Loops through the pl-pl collision list and groups families together by index. Outputs the indices of all family members, + !! Loops through the pl-pl collision list and groups families together by index. Outputs the indices of all colliders%idx members, !! and pairs of quantities (x and v vectors, mass, radius, L_spin, and Ip) that can be used to resolve the collisional outcome. implicit none ! Arguments class(symba_pl), intent(inout) :: pl !! SyMBA massive body object + class(symba_cb), intent(inout) :: cb !! SyMBA central body object class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions integer(I4B), dimension(2), intent(inout) :: idx_parent !! Index of the two bodies considered the "parents" of the collision - integer(I4B), dimension(:), allocatable, intent(out) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(NDIM,2), intent(out) :: x, v, L_spin, Ip !! Output values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(2), intent(out) :: mass, radius !! Output values that represent a 2-body equivalent of a possibly 2+ body collision + class(fraggle_colliders), intent(out) :: colliders ! Result - logical :: lflag !! Logical flag indicating whether a family was successfully created or not + logical :: lflag !! Logical flag indicating whether a colliders%idx was successfully created or not ! Internals - type family_array + type collidx_array integer(I4B), dimension(:), allocatable :: id integer(I4B), dimension(:), allocatable :: idx - end type family_array - type(family_array), dimension(2) :: parent_child_index_array + end type collidx_array + type(collidx_array), dimension(2) :: parent_child_index_array integer(I4B), dimension(2) :: nchild - integer(I4B) :: i, j, fam_size, idx_child + integer(I4B) :: i, j, ncolliders, idx_child real(DP), dimension(2) :: volume, density real(DP) :: mchild, mtot, volchild real(DP), dimension(NDIM) :: xc, vc, xcom, vcom, xchild, vchild, xcrossv + real(DP), dimension(NDIM,2) :: mxc, vcc nchild(:) = pl%kin(idx_parent(:))%nchild ! If all of these bodies share a parent, but this is still a unique collision, move the last child @@ -176,6 +456,7 @@ function symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v if (idx_parent(1) == idx_parent(2)) then if (nchild(1) == 0) then ! There is only one valid body recorded in this pair (this could happen due to restructuring of the kinship relationships, though it should be rare) lflag = .false. + call pl%reset_kinship([idx_parent(1)]) return end if idx_parent(2) = pl%kin(idx_parent(1))%child(nchild(1)) @@ -185,9 +466,9 @@ function symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v pl%kin(idx_parent(2))%parent = idx_parent(1) end if - mass(:) = pl%mass(idx_parent(:)) ! Note: This is meant to mass, not G*mass, as the collisional regime determination uses mass values that will be converted to Si - radius(:) = pl%radius(idx_parent(:)) - volume(:) = (4.0_DP / 3.0_DP) * PI * radius(:)**3 + colliders%mass(:) = pl%mass(idx_parent(:)) ! Note: This is meant to mass, not G*mass, as the collisional regime determination uses mass values that will be converted to Si + colliders%radius(:) = pl%radius(idx_parent(:)) + volume(:) = (4.0_DP / 3.0_DP) * PI * colliders%radius(:)**3 ! Group together the ids and indexes of each collisional parent and its children do j = 1, 2 @@ -204,23 +485,24 @@ function symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v end associate end do - ! Consolidate the groups of collsional parents with any children they may have into a single "family" index array - fam_size = 2 + sum(nchild(:)) - allocate(family(fam_size)) - family = [parent_child_index_array(1)%idx(:),parent_child_index_array(2)%idx(:)] - fam_size = count(pl%lcollision(family(:))) - family = pack(family(:), pl%lcollision(family(:))) - L_spin(:,:) = 0.0_DP - Ip(:,:) = 0.0_DP + ! Consolidate the groups of collsional parents with any children they may have into a single "colliders%idx" index array + ncolliders = 2 + sum(nchild(:)) + allocate(colliders%idx(ncolliders)) + colliders%idx = [parent_child_index_array(1)%idx(:),parent_child_index_array(2)%idx(:)] + + colliders%ncoll = count(pl%lcollision(colliders%idx(:))) + colliders%idx = pack(colliders%idx(:), pl%lcollision(colliders%idx(:))) + colliders%L_spin(:,:) = 0.0_DP + colliders%Ip(:,:) = 0.0_DP ! Find the barycenter of each body along with its children, if it has any do j = 1, 2 - x(:, j) = pl%xb(:, idx_parent(j)) - v(:, j) = pl%vb(:, idx_parent(j)) + colliders%xb(:, j) = pl%xh(:, idx_parent(j)) + cb%xb(:) + colliders%vb(:, j) = pl%vb(:, idx_parent(j)) ! Assume principal axis rotation about axis corresponding to highest moment of inertia (3rd Ip) if (param%lrotation) then - Ip(:, j) = mass(j) * pl%Ip(:, idx_parent(j)) - L_spin(:, j) = Ip(3, j) * radius(j)**2 * pl%rot(:, idx_parent(j)) + colliders%Ip(:, j) = colliders%mass(j) * pl%Ip(:, idx_parent(j)) + colliders%L_spin(:, j) = colliders%Ip(3, j) * colliders%radius(j)**2 * pl%rot(:, idx_parent(j)) end if if (nchild(j) > 0) then @@ -228,46 +510,57 @@ function symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v idx_child = parent_child_index_array(j)%idx(i + 1) if (.not. pl%lcollision(idx_child)) cycle mchild = pl%mass(idx_child) - xchild(:) = pl%xb(:, idx_child) + xchild(:) = pl%xh(:, idx_child) + cb%xb(:) vchild(:) = pl%vb(:, idx_child) volchild = (4.0_DP / 3.0_DP) * PI * pl%radius(idx_child)**3 volume(j) = volume(j) + volchild ! Get angular momentum of the child-parent pair and add that to the spin ! Add the child's spin if (param%lrotation) then - xcom(:) = (mass(j) * x(:,j) + mchild * xchild(:)) / (mass(j) + mchild) - vcom(:) = (mass(j) * v(:,j) + mchild * vchild(:)) / (mass(j) + mchild) - xc(:) = x(:, j) - xcom(:) - vc(:) = v(:, j) - vcom(:) + xcom(:) = (colliders%mass(j) * colliders%xb(:,j) + mchild * xchild(:)) / (colliders%mass(j) + mchild) + vcom(:) = (colliders%mass(j) * colliders%vb(:,j) + mchild * vchild(:)) / (colliders%mass(j) + mchild) + xc(:) = colliders%xb(:, j) - xcom(:) + vc(:) = colliders%vb(:, j) - vcom(:) xcrossv(:) = xc(:) .cross. vc(:) - L_spin(:, j) = L_spin(:, j) + mass(j) * xcrossv(:) + colliders%L_spin(:, j) = colliders%L_spin(:, j) + colliders%mass(j) * xcrossv(:) xc(:) = xchild(:) - xcom(:) vc(:) = vchild(:) - vcom(:) xcrossv(:) = xc(:) .cross. vc(:) - L_spin(:, j) = L_spin(:, j) + mchild * xcrossv(:) + colliders%L_spin(:, j) = colliders%L_spin(:, j) + mchild * xcrossv(:) - L_spin(:, j) = L_spin(:, j) + mchild * pl%Ip(3, idx_child) * pl%radius(idx_child)**2 * pl%rot(:, idx_child) - Ip(:, j) = Ip(:, j) + mchild * pl%Ip(:, idx_child) + colliders%L_spin(:, j) = colliders%L_spin(:, j) + mchild * pl%Ip(3, idx_child) * pl%radius(idx_child)**2 * pl%rot(:, idx_child) + colliders%Ip(:, j) = colliders%Ip(:, j) + mchild * pl%Ip(:, idx_child) end if ! Merge the child and parent - mass(j) = mass(j) + mchild - x(:, j) = xcom(:) - v(:, j) = vcom(:) + colliders%mass(j) = colliders%mass(j) + mchild + colliders%xb(:, j) = xcom(:) + colliders%vb(:, j) = vcom(:) end do end if - density(j) = mass(j) / volume(j) - radius(j) = ((3 * mass(j)) / (density(j) * 4 * pi))**(1.0_DP / 3.0_DP) - if (param%lrotation) Ip(:, j) = Ip(:, j) / mass(j) + density(j) = colliders%mass(j) / volume(j) + colliders%radius(j) = (3 * volume(j) / (4 * PI))**(1.0_DP / 3.0_DP) + if (param%lrotation) colliders%Ip(:, j) = colliders%Ip(:, j) / colliders%mass(j) + + xcom(:) = (colliders%mass(1) * colliders%xb(:, 1) + colliders%mass(2) * colliders%xb(:, 2)) / sum(colliders%mass(:)) + vcom(:) = (colliders%mass(1) * colliders%vb(:, 1) + colliders%mass(2) * colliders%vb(:, 2)) / sum(colliders%mass(:)) + mxc(:, 1) = colliders%mass(1) * (colliders%xb(:, 1) - xcom(:)) + mxc(:, 2) = colliders%mass(2) * (colliders%xb(:, 2) - xcom(:)) + vcc(:, 1) = colliders%vb(:, 1) - vcom(:) + vcc(:, 2) = colliders%vb(:, 2) - vcom(:) + colliders%L_orbit(:,:) = mxc(:,:) .cross. vcc(:,:) end do lflag = .true. + ! Destroy the kinship relationships for all members of this colliders%idx + call pl%reset_kinship(colliders%idx(:)) + return - end function symba_collision_consolidate_familes + end function symba_collision_consolidate_colliders - module subroutine symba_collision_encounter_scrub(self, system, param) + module subroutine symba_collision_encounter_extract_collisions(self, system, param) !! author: David A. Minton !! !! Processes the pl-pl encounter list remove only those encounters that led to a collision @@ -278,67 +571,68 @@ module subroutine symba_collision_encounter_scrub(self, system, param) class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters ! Internals - logical, dimension(self%nenc) :: lplpl_collision + logical, dimension(:), allocatable :: lplpl_collision logical, dimension(:), allocatable :: lplpl_unique_parent integer(I4B), dimension(:), pointer :: plparent integer(I4B), dimension(:), allocatable :: collision_idx, unique_parent_idx - integer(I4B) :: i, index_coll, ncollisions, nunique_parent - type(symba_plplenc) :: plplenc_noncollision + integer(I4B) :: i, index_coll, ncollisions, nunique_parent, nplplenc select type (pl => system%pl) class is (symba_pl) - associate(plplenc_list => self, nplplenc => self%nenc, idx1 => self%index1, idx2 => self%index2, plparent => pl%kin%parent) + associate(plplenc_list => self, idx1 => self%index1, idx2 => self%index2, plparent => pl%kin%parent) + nplplenc = plplenc_list%nenc + allocate(lplpl_collision(nplplenc)) lplpl_collision(:) = plplenc_list%status(1:nplplenc) == COLLISION - if (any(lplpl_collision)) then ! Collisions have been detected in this step. So we need to determine which of them are between unique bodies. - - ! Get the subset of pl-pl encounters that lead to a collision - ncollisions = count(lplpl_collision(:)) - allocate(collision_idx(ncollisions)) - collision_idx = pack([(i, i=1, nplplenc)], lplpl_collision) - - ! Get the subset of collisions that involve a unique pair of parents - allocate(lplpl_unique_parent(ncollisions)) - - lplpl_unique_parent(:) = plparent(idx1(collision_idx(:))) /= plparent(idx2(collision_idx(:))) - nunique_parent = count(lplpl_unique_parent(:)) - allocate(unique_parent_idx(nunique_parent)) - unique_parent_idx = pack(collision_idx(:), lplpl_unique_parent(:)) - - ! Scrub all pl-pl collisions involving unique pairs of parents, which will remove all duplicates and leave behind - ! all pairs that have themselves as parents but are not part of the unique parent list. This can hapepn in rare cases - ! due to restructuring of parent/child relationships when there are large numbers of multi-body collisions in a single - ! step - lplpl_unique_parent(:) = .true. - do index_coll = 1, ncollisions - associate(ip1 => plparent(idx1(collision_idx(index_coll))), ip2 => plparent(idx2(collision_idx(index_coll)))) - lplpl_unique_parent(:) = .not. ( any(plparent(idx1(unique_parent_idx(:))) == ip1) .or. & - any(plparent(idx2(unique_parent_idx(:))) == ip1) .or. & - any(plparent(idx1(unique_parent_idx(:))) == ip2) .or. & - any(plparent(idx2(unique_parent_idx(:))) == ip2) ) - end associate - end do + if (.not.any(lplpl_collision)) return + ! Collisions have been detected in this step. So we need to determine which of them are between unique bodies. - ! Reassemble collision index list to include only those containing the unique pairs of parents, plus all the non-unique pairs that don't - ! contain a parent body on the unique parent list. - ncollisions = nunique_parent + count(lplpl_unique_parent) - collision_idx = [unique_parent_idx(:), pack(collision_idx(:), lplpl_unique_parent(:))] + ! Get the subset of pl-pl encounters that lead to a collision + ncollisions = count(lplpl_collision(:)) + allocate(collision_idx(ncollisions)) + collision_idx = pack([(i, i=1, nplplenc)], lplpl_collision) - ! Create a mask that contains only the pl-pl encounters that did not result in a collision, and then discard them - lplpl_collision(:) = .false. - lplpl_collision(collision_idx(:)) = .true. - end if - call plplenc_list%spill(plplenc_noncollision, .not.lplpl_collision, ldestructive=.true.) ! Remove any encounters that are not collisions from the list. + ! Get the subset of collisions that involve a unique pair of parents + allocate(lplpl_unique_parent(ncollisions)) + + lplpl_unique_parent(:) = plparent(idx1(collision_idx(:))) /= plparent(idx2(collision_idx(:))) + nunique_parent = count(lplpl_unique_parent(:)) + allocate(unique_parent_idx(nunique_parent)) + unique_parent_idx = pack(collision_idx(:), lplpl_unique_parent(:)) + + ! Scrub all pl-pl collisions involving unique pairs of parents, which will remove all duplicates and leave behind + ! all pairs that have themselves as parents but are not part of the unique parent list. This can hapepn in rare cases + ! due to restructuring of parent/child relationships when there are large numbers of multi-body collisions in a single + ! step + lplpl_unique_parent(:) = .true. + do index_coll = 1, ncollisions + associate(ip1 => plparent(idx1(collision_idx(index_coll))), ip2 => plparent(idx2(collision_idx(index_coll)))) + lplpl_unique_parent(:) = .not. ( any(plparent(idx1(unique_parent_idx(:))) == ip1) .or. & + any(plparent(idx2(unique_parent_idx(:))) == ip1) .or. & + any(plparent(idx1(unique_parent_idx(:))) == ip2) .or. & + any(plparent(idx2(unique_parent_idx(:))) == ip2) ) + end associate + end do + + ! Reassemble collision index list to include only those containing the unique pairs of parents, plus all the non-unique pairs that don't + ! contain a parent body on the unique parent list. + ncollisions = nunique_parent + count(lplpl_unique_parent) + collision_idx = [unique_parent_idx(:), pack(collision_idx(:), lplpl_unique_parent(:))] + + ! Create a mask that contains only the pl-pl encounters that did not result in a collision, and then discard them + lplpl_collision(:) = .false. + lplpl_collision(collision_idx(:)) = .true. + call plplenc_list%spill(system%plplcollision_list, lplpl_collision, ldestructive=.true.) ! Extract any encounters that are not collisions from the list. end associate end select return - end subroutine symba_collision_encounter_scrub + end subroutine symba_collision_encounter_extract_collisions - module subroutine symba_collision_make_family_pl(self, idx) + module subroutine symba_collision_make_colliders_pl(self, idx) !! author: Jennifer L.L. Pouplin, Carlisle A. wishard, and David A. Minton !! - !! When a single body is involved in more than one collision in a single step, it becomes part of a family. + !! When a single body is involved in more than one collision in a single step, it becomes part of a colliders%idx. !! The largest body involved in a multi-body collision is the "parent" and all bodies that collide with it are its "children," !! including those that collide with the children. !! @@ -383,8 +677,7 @@ module subroutine symba_collision_make_family_pl(self, idx) pl%kin(j)%parent = index_parent end do end if - if (allocated(pl%kin(index_child)%child)) deallocate(pl%kin(index_child)%child) - pl%kin(index_child)%nchild = 0 + call pl%reset_kinship([index_child]) ! Add the new child to its parent pl%kin(index_child)%parent = index_parent temp(nchild_new) = index_child @@ -394,7 +687,167 @@ module subroutine symba_collision_make_family_pl(self, idx) end associate return - end subroutine symba_collision_make_family_pl + end subroutine symba_collision_make_colliders_pl + + + subroutine symba_collision_mergeaddsub(system, param, colliders, frag, status) + !! author: David A. Minton + !! + !! Fills the pl_discards and pl_adds with removed and added bodies + !! + implicit none + ! Arguments + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + class(fraggle_colliders), intent(inout) :: colliders !! Fraggle colliders object + class(fraggle_fragments), intent(inout) :: frag !! Fraggle fragmentation system object + integer(I4B), intent(in) :: status !! Status flag to assign to adds + ! Internals + integer(I4B) :: i, ibiggest, ismallest, iother, nstart, nend, ncolliders, nfrag + logical, dimension(system%pl%nbody) :: lmask + class(symba_pl), allocatable :: plnew, plsub + character(*), parameter :: FRAGFMT = '("Newbody",I0.7)' + character(len=NAMELEN) :: newname + character(len=STRMAX) :: message + + select type(pl => system%pl) + class is (symba_pl) + select type(pl_discards => system%pl_discards) + class is (symba_merger) + associate(info => pl%info, pl_adds => system%pl_adds, cb => system%cb, npl => pl%nbody) + ! Add the colliders%idx bodies to the subtraction list + ncolliders = colliders%ncoll + nfrag = frag%nbody + + ! Setup new bodies + allocate(plnew, mold=pl) + call plnew%setup(nfrag, param) + ibiggest = colliders%idx(maxloc(pl%Gmass(colliders%idx(:)), dim=1)) + ismallest = colliders%idx(minloc(pl%Gmass(colliders%idx(:)), dim=1)) + + ! Copy over identification, information, and physical properties of the new bodies from the fragment list + plnew%id(1:nfrag) = frag%id(1:nfrag) + plnew%xb(:, 1:nfrag) = frag%xb(:, 1:nfrag) + plnew%vb(:, 1:nfrag) = frag%vb(:, 1:nfrag) + call pl%vb2vh(cb) + call pl%xh2xb(cb) + do i = 1, nfrag + plnew%xh(:,i) = frag%xb(:, i) - cb%xb(:) + plnew%vh(:,i) = frag%vb(:, i) - cb%vb(:) + end do + plnew%mass(1:nfrag) = frag%mass(1:nfrag) + plnew%Gmass(1:nfrag) = param%GU * frag%mass(1:nfrag) + plnew%radius(1:nfrag) = frag%radius(1:nfrag) + plnew%density(1:nfrag) = frag%mass(1:nfrag) / frag%radius(1:nfrag) + call plnew%set_rhill(cb) + + select case(status) + case(DISRUPTION) + plnew%status(1:nfrag) = NEW_PARTICLE + do i = 1, nfrag + write(newname, FRAGFMT) frag%id(i) + call plnew%info(i)%set_value(origin_type="Disruption", origin_time=param%t, name=newname, origin_xh=plnew%xh(:,i), origin_vh=plnew%vh(:,i)) + end do + do i = 1, ncolliders + if (colliders%idx(i) == ibiggest) then + iother = ismallest + else + iother = ibiggest + end if + call pl%info(colliders%idx(i))%set_value(status="Disruption", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=iother) + end do + case(SUPERCATASTROPHIC) + plnew%status(1:nfrag) = NEW_PARTICLE + do i = 1, nfrag + write(newname, FRAGFMT) frag%id(i) + call plnew%info(i)%set_value(origin_type="Supercatastrophic", origin_time=param%t, name=newname, origin_xh=plnew%xh(:,i), origin_vh=plnew%vh(:,i)) + end do + do i = 1, ncolliders + if (colliders%idx(i) == ibiggest) then + iother = ismallest + else + iother = ibiggest + end if + call pl%info(colliders%idx(i))%set_value(status="Supercatastrophic", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=iother) + end do + case(HIT_AND_RUN_DISRUPT) + call plnew%info(1)%copy(pl%info(ibiggest)) + plnew%status(1) = OLD_PARTICLE + do i = 2, nfrag + write(newname, FRAGFMT) frag%id(i) + call plnew%info(i)%set_value(origin_type="Hit and run fragment", origin_time=param%t, name=newname, origin_xh=plnew%xh(:,i), origin_vh=plnew%vh(:,i)) + end do + do i = 1, ncolliders + if (colliders%idx(i) == ibiggest) cycle + iother = ibiggest + call pl%info(colliders%idx(i))%set_value(status="Hit and run fragmention", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=iother) + end do + case(MERGED) + call plnew%info(1)%copy(pl%info(ibiggest)) + plnew%status(1) = OLD_PARTICLE + do i = 1, ncolliders + if (colliders%idx(i) == ibiggest) cycle + + iother = ibiggest + call pl%info(colliders%idx(i))%set_value(status="MERGED", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=iother) + end do + end select + + if (param%lrotation) then + plnew%Ip(:, 1:nfrag) = frag%Ip(:, 1:nfrag) + plnew%rot(:, 1:nfrag) = frag%rot(:, 1:nfrag) + end if + + if (param%ltides) then + plnew%Q = pl%Q(ibiggest) + plnew%k2 = pl%k2(ibiggest) + plnew%tlag = pl%tlag(ibiggest) + end if + + !Copy over or set integration parameters for new bodies + plnew%lcollision(1:nfrag) = .false. + plnew%ldiscard(1:nfrag) = .false. + plnew%levelg(1:nfrag) = pl%levelg(ibiggest) + plnew%levelm(1:nfrag) = pl%levelm(ibiggest) + + ! Log the properties of the new bodies + call fraggle_io_log_pl(plnew, param) + + ! Append the new merged body to the list + nstart = pl_adds%nbody + 1 + nend = pl_adds%nbody + nfrag + call pl_adds%append(plnew, lsource_mask=[(.true., i=1, nfrag)]) + ! Record how many bodies were added in this event + pl_adds%ncomp(nstart:nend) = plnew%nbody + + ! Add the discarded bodies to the discard list + pl%status(colliders%idx(:)) = MERGED + pl%ldiscard(colliders%idx(:)) = .true. + pl%lcollision(colliders%idx(:)) = .true. + lmask(:) = .false. + lmask(colliders%idx(:)) = .true. + + call plnew%setup(0, param) + deallocate(plnew) + + allocate(plsub, mold=pl) + call pl%spill(plsub, lmask, ldestructive=.false.) + + nstart = pl_discards%nbody + 1 + nend = pl_discards%nbody + ncolliders + call pl_discards%append(plsub, lsource_mask=[(.true., i = 1, ncolliders)]) + + ! Record how many bodies were subtracted in this event + pl_discards%ncomp(nstart:nend) = ncolliders + + call plsub%setup(0, param) + deallocate(plsub) + end associate + end select + end select + + return + end subroutine symba_collision_mergeaddsub module subroutine symba_collision_resolve_fragmentations(self, system, param) @@ -406,80 +859,43 @@ module subroutine symba_collision_resolve_fragmentations(self, system, param) ! Arguments class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions ! Internals ! Internals - integer(I4B), dimension(:), allocatable :: family !! List of indices of all bodies inovlved in the collision integer(I4B), dimension(2) :: idx_parent !! Index of the two bodies considered the "parents" of the collision real(DP), dimension(NDIM,2) :: x, v, L_spin, Ip !! Output values that represent a 2-body equivalent of a possibly 2+ body collision real(DP), dimension(2) :: mass, radius !! Output values that represent a 2-body equivalent of a possibly 2+ body collision logical :: lgoodcollision - integer(I4B) :: i, status, jtarg, jproj, regime - real(DP), dimension(2) :: radius_si, mass_si, density_si - real(DP) :: mtiny_si, Mcb_si - real(DP), dimension(NDIM) :: x1_si, v1_si, x2_si, v2_si - real(DP) :: mlr, mslr, mtot, dentot, msys, msys_new, Qloss, impact_parameter - integer(I4B), parameter :: NRES = 3 !! Number of collisional product results - real(DP), dimension(NRES) :: mass_res - - associate(plpl_collisions => self, ncollisions => self%nenc, idx1 => self%index1, idx2 => self%index2, cb => system%cb) + integer(I4B) :: i + type(fraggle_colliders) :: colliders !! Fraggle colliders object + type(fraggle_fragments) :: frag !! Fraggle fragmentation system object + + associate(plplcollision_list => self, ncollisions => self%nenc, idx1 => self%index1, idx2 => self%index2) select type(pl => system%pl) class is (symba_pl) - do i = 1, ncollisions - idx_parent(1) = pl%kin(idx1(i))%parent - idx_parent(2) = pl%kin(idx2(i))%parent - lgoodcollision = symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v, mass, radius, L_spin, Ip) - if (.not. lgoodcollision) cycle - if (any(pl%status(idx_parent(:)) /= COLLISION)) cycle ! One of these two bodies has already been resolved - - ! Convert all quantities to SI units and determine which of the pair is the projectile vs. target before sending them - ! to symba_regime - if (mass(1) > mass(2)) then - jtarg = 1 - jproj = 2 - else - jtarg = 2 - jproj = 1 - end if - mass_si(:) = (mass(:)) * param%MU2KG !! The collective mass of the parent and its children - radius_si(:) = radius(:) * param%DU2M !! The collective radius of the parent and its children - x1_si(:) = plpl_collisions%x1(:,i) * param%DU2M !! The position of the parent from inside the step (at collision) - v1_si(:) = plpl_collisions%v1(:,i) * param%DU2M / param%TU2S !! The velocity of the parent from inside the step (at collision) - x2_si(:) = plpl_collisions%x2(:,i) * param%DU2M !! The position of the parent from inside the step (at collision) - v2_si(:) = plpl_collisions%v2(:,i) * param%DU2M / param%TU2S !! The velocity of the parent from inside the step (at collision) - density_si(:) = mass_si(:) / (4.0_DP / 3._DP * PI * radius_si(:)**3) !! The collective density of the parent and its children - Mcb_si = cb%mass * param%MU2KG - mtiny_si = (param%GMTINY / param%GU) * param%MU2KG - - mass_res(:) = 0.0_DP - - mtot = sum(mass_si(:)) - dentot = sum(mass_si(:) * density_si(:)) / mtot - - !! Use the positions and velocities of the parents from indside the step (at collision) to calculate the collisional regime - call fragmentation_regime(Mcb_si, mass_si(jtarg), mass_si(jproj), radius_si(jtarg), radius_si(jproj), x1_si(:), x2_si(:),& - v1_si(:), v2_si(:), density_si(jtarg), density_si(jproj), regime, mlr, mslr, mtiny_si, Qloss) - - mass_res(1) = min(max(mlr, 0.0_DP), mtot) - mass_res(2) = min(max(mslr, 0.0_DP), mtot) - mass_res(3) = min(max(mtot - mlr - mslr, 0.0_DP), mtot) - mass_res(:) = (mass_res(:) / param%MU2KG) - Qloss = Qloss * (param%TU2S / param%DU2M)**2 / param%MU2KG - - select case (regime) - case (COLLRESOLVE_REGIME_DISRUPTION) - status = symba_fragmentation_casedisruption(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) - case (COLLRESOLVE_REGIME_SUPERCATASTROPHIC) - status = symba_fragmentation_casesupercatastrophic(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) - case (COLLRESOLVE_REGIME_HIT_AND_RUN) - status = symba_fragmentation_casehitandrun(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) - case (COLLRESOLVE_REGIME_MERGE, COLLRESOLVE_REGIME_GRAZE_AND_MERGE) - status = symba_fragmentation_casemerge(system, param, family, x, v, mass, radius, L_spin, Ip) - case default - write(*,*) "Error in symba_collision, unrecognized collision regime" - call util_exit(FAILURE) - end select - end do + select type (cb => system%cb) + class is (symba_cb) + do i = 1, ncollisions + idx_parent(1) = pl%kin(idx1(i))%parent + idx_parent(2) = pl%kin(idx2(i))%parent + lgoodcollision = symba_collision_consolidate_colliders(pl, cb, param, idx_parent, colliders) + if ((.not. lgoodcollision) .or. any(pl%status(idx_parent(:)) /= COLLISION)) cycle + + call colliders%regime(frag, system, param) + + select case (frag%regime) + case (COLLRESOLVE_REGIME_DISRUPTION, COLLRESOLVE_REGIME_SUPERCATASTROPHIC) + plplcollision_list%status(i) = symba_collision_casedisruption(system, param, colliders, frag) + case (COLLRESOLVE_REGIME_HIT_AND_RUN) + plplcollision_list%status(i) = symba_collision_casehitandrun(system, param, colliders, frag) + case (COLLRESOLVE_REGIME_MERGE, COLLRESOLVE_REGIME_GRAZE_AND_MERGE) + plplcollision_list%status(i) = symba_collision_casemerge(system, param, colliders, frag) + case default + write(*,*) "Error in symba_collision, unrecognized collision regime" + call util_exit(FAILURE) + end select + end do + end select end select end associate @@ -496,30 +912,145 @@ module subroutine symba_collision_resolve_mergers(self, system, param) ! Arguments class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions ! Internals - integer(I4B), dimension(:), allocatable :: family !! List of indices of all bodies inovlved in the collision integer(I4B), dimension(2) :: idx_parent !! Index of the two bodies considered the "parents" of the collision real(DP), dimension(NDIM,2) :: x, v, L_spin, Ip !! Output values that represent a 2-body equivalent of a possibly 2+ body collision real(DP), dimension(2) :: mass, radius !! Output values that represent a 2-body equivalent of a possibly 2+ body collision logical :: lgoodcollision - integer(I4B) :: i, status + integer(I4B) :: i + type(fraggle_colliders) :: colliders !! Fraggle colliders object + type(fraggle_fragments) :: frag !! Fraggle fragmentation system object - associate(plpl_collisions => self, ncollisions => self%nenc, idx1 => self%index1, idx2 => self%index2) + associate(plplcollision_list => self, ncollisions => self%nenc, idx1 => self%index1, idx2 => self%index2) select type(pl => system%pl) class is (symba_pl) - do i = 1, ncollisions - idx_parent(1) = pl%kin(idx1(i))%parent - idx_parent(2) = pl%kin(idx2(i))%parent - lgoodcollision = symba_collision_consolidate_familes(pl, param, idx_parent, family, x, v, mass, radius, L_spin, Ip) - if (.not. lgoodcollision) cycle - if (any(pl%status(idx_parent(:)) /= COLLISION)) cycle ! One of these two bodies has already been resolved - status = symba_fragmentation_casemerge(system, param, family, x, v, mass, radius, L_spin, Ip) - end do + select type(cb => system%cb) + class is (symba_cb) + do i = 1, ncollisions + idx_parent(1) = pl%kin(idx1(i))%parent + idx_parent(2) = pl%kin(idx2(i))%parent + lgoodcollision = symba_collision_consolidate_colliders(pl, cb, param, idx_parent, colliders) + if (.not. lgoodcollision) cycle + if (any(pl%status(idx_parent(:)) /= COLLISION)) cycle ! One of these two bodies has already been resolved + + frag%regime = COLLRESOLVE_REGIME_MERGE + frag%mtot = sum(colliders%mass(:)) + frag%xbcom(:) = (colliders%mass(1) * colliders%xb(:,1) + colliders%mass(2) * colliders%xb(:,2)) / frag%mtot + frag%vbcom(:) = (colliders%mass(1) * colliders%vb(:,1) + colliders%mass(2) * colliders%vb(:,2)) / frag%mtot + plplcollision_list%status(i) = symba_collision_casemerge(system, param, colliders, frag) + end do + end select end select end associate return end subroutine symba_collision_resolve_mergers + + module subroutine symba_collision_resolve_plplenc(self, system, param, t, dt, irec) + !! author: David A. Minton + !! + !! Process the pl-pl collision list, then modifiy the massive bodies based on the outcome of the collision + !! + implicit none + ! Arguments + class(symba_plplenc), intent(inout) :: self !! SyMBA pl-pl encounter list + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + real(DP), intent(in) :: t !! Current simulation time + real(DP), intent(in) :: dt !! Current simulation step size + integer(I4B), intent(in) :: irec !! Current recursion level + ! Internals + real(DP) :: Eorbit_before, Eorbit_after + logical :: lplpl_collision + character(len=STRMAX) :: timestr + class(symba_parameters), allocatable :: tmp_param + + associate(plplenc_list => self, plplcollision_list => system%plplcollision_list) + select type(pl => system%pl) + class is (symba_pl) + select type(param) + class is (symba_parameters) + if (plplcollision_list%nenc == 0) return ! No collisions to resolve + ! Make sure that the heliocentric and barycentric coordinates are consistent with each other + call pl%vb2vh(system%cb) + call pl%xh2xb(system%cb) + + ! Get the energy before the collision is resolved + if (param%lenergy) then + call system%get_energy_and_momentum(param) + Eorbit_before = system%te + end if + + do + write(timestr,*) t + call fraggle_io_log_one_message("") + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message("Collision between massive bodies detected at time t = " // trim(adjustl(timestr))) + call fraggle_io_log_one_message("***********************************************************************************************************************") + allocate(tmp_param, source=param) + tmp_param%t = t + if (param%lfragmentation) then + call plplcollision_list%resolve_fragmentations(system, param) + else + call plplcollision_list%resolve_mergers(system, param) + end if + + ! Destroy the collision list now that the collisions are resolved + call plplcollision_list%setup(0) + + if ((system%pl_adds%nbody == 0) .and. (system%pl_discards%nbody == 0)) exit + + ! Save the add/discard information to file + call system%write_discard(tmp_param) + + ! Rearrange the arrays: Remove discarded bodies, add any new bodies, resort, and recompute all indices and encounter lists + call pl%rearray(system, tmp_param) + + ! Destroy the add/discard list so that we don't append the same body multiple times if another collision is detected + call system%pl_discards%setup(0, param) + call system%pl_adds%setup(0, param) + deallocate(tmp_param) + + ! Check whether or not any of the particles that were just added are themselves in a collision state. This will generate a new plplcollision_list + lplpl_collision = plplenc_list%collision_check(system, param, t, dt, irec) + + if (.not.lplpl_collision) exit + end do + + if (param%lenergy) then + call system%get_energy_and_momentum(param) + Eorbit_after = system%te + param%Ecollisions = param%Ecollisions + (Eorbit_after - Eorbit_before) + end if + + end select + end select + end associate + + return + end subroutine symba_collision_resolve_plplenc + + + module subroutine symba_collision_resolve_pltpenc(self, system, param, t, dt, irec) + !! author: David A. Minton + !! + !! Process the pl-tp collision list, then modifiy the massive bodies based on the outcome of the collision + !! + implicit none + ! Arguments + class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-pl encounter list + class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA additions + real(DP), intent(in) :: t !! Current simulation tim + real(DP), intent(in) :: dt !! Current simulation step size + integer(I4B), intent(in) :: irec !! Current recursion level + + call system%tp%xh2xb(system%cb) + call system%tp%discard(system, param) + + return + end subroutine symba_collision_resolve_pltpenc + end submodule s_symba_collision \ No newline at end of file diff --git a/src/symba/symba_discard.f90 b/src/symba/symba_discard.f90 index c154b4290..704d11f85 100644 --- a/src/symba/symba_discard.f90 +++ b/src/symba/symba_discard.f90 @@ -20,6 +20,7 @@ subroutine symba_discard_cb_pl(pl, system, param) ! Internals integer(I4B) :: i, j real(DP) :: energy, vb2, rb2, rh2, rmin2, rmax2, rmaxu2 + character(len=STRMAX) :: idstr, timestr, message associate(npl => pl%nbody, cb => system%cb) call system%set_msys() @@ -33,12 +34,28 @@ subroutine symba_discard_cb_pl(pl, system, param) pl%ldiscard(i) = .true. pl%lcollision(i) = .false. pl%status(i) = DISCARDED_RMAX - write(*, *) "Massive body ", pl%id(i), " too far from the central body at t = ", param%t + write(idstr, *) pl%id(i) + write(timestr, *) param%t + write(message, *) trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " too far from the central body at t = " // trim(adjustl(timestr)) + call fraggle_io_log_one_message("") + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message(message) + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message("") + call pl%info(i)%set_value(status="DISCARDED_RMAX", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i)) else if ((param%rmin >= 0.0_DP) .and. (rh2 < rmin2)) then pl%ldiscard(i) = .true. pl%lcollision(i) = .false. pl%status(i) = DISCARDED_RMIN - write(*, *) "Massive body ", pl%id(i), " too close to the central body at t = ", param%t + write(idstr, *) pl%id(i) + write(timestr, *) param%t + write(message, *) trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " too close to the central body at t = " // trim(adjustl(timestr)) + call fraggle_io_log_one_message("") + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message(message) + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message("") + call pl%info(i)%set_value(status="DISCARDED_RMIN", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=cb%id) else if (param%rmaxu >= 0.0_DP) then rb2 = dot_product(pl%xb(:,i), pl%xb(:,i)) vb2 = dot_product(pl%vb(:,i), pl%vb(:,i)) @@ -47,7 +64,15 @@ subroutine symba_discard_cb_pl(pl, system, param) pl%ldiscard(i) = .true. pl%lcollision(i) = .false. pl%status(i) = DISCARDED_RMAXU - write(*, *) "Massive body ", pl%id(i), " is unbound and too far from barycenter at t = ", param%t + write(idstr, *) pl%id(i) + write(timestr, *) param%t + write(message, *) trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstr)) // ")" // " is unbound and too far from barycenter at t = " // trim(adjustl(timestr)) + call fraggle_io_log_one_message("") + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message(message) + call fraggle_io_log_one_message("***********************************************************************************************************************") + call fraggle_io_log_one_message("") + call pl%info(i)%set_value(status="DISCARDED_RMAXU", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i)) end if end if end if @@ -78,7 +103,7 @@ subroutine symba_discard_conserve_mtm(pl, system, param, ipl, lescape_body) class is (symba_cb) ! Add the potential and kinetic energy of the lost body to the records - pe = -cb%mass * pl%mass(ipl) / norm2(pl%xb(:, ipl) - cb%xb(:)) + pe = -cb%Gmass * pl%mass(ipl) / norm2(pl%xb(:, ipl) - cb%xb(:)) ke_orbit = 0.5_DP * pl%mass(ipl) * dot_product(pl%vb(:, ipl), pl%vb(:, ipl)) if (param%lrotation) then ke_spin = 0.5_DP * pl%mass(ipl) * pl%radius(ipl)**2 * pl%Ip(3, ipl) * dot_product(pl%rot(:, ipl), pl%rot(:, ipl)) @@ -89,18 +114,18 @@ subroutine symba_discard_conserve_mtm(pl, system, param, ipl, lescape_body) ! Add the pre-collision ke of the central body to the records ! Add planet mass to central body accumulator if (lescape_body) then - system%Mescape = system%Mescape + pl%mass(ipl) + param%GMescape = param%GMescape + pl%Gmass(ipl) do i = 1, pl%nbody if (i == ipl) cycle - pe = pe - pl%mass(i) * pl%mass(ipl) / norm2(pl%xb(:, ipl) - pl%xb(:, i)) + pe = pe - pl%Gmass(i) * pl%mass(ipl) / norm2(pl%xb(:, ipl) - pl%xb(:, i)) end do Ltot(:) = 0.0_DP do i = 1, pl%nbody - Lpl(:) = pL%mass(i) * pl%xb(:,i) .cross. pl%vb(:, i) + Lpl(:) = pL%mass(i) * (pl%xb(:,i) .cross. pl%vb(:, i)) Ltot(:) = Ltot(:) + Lpl(:) end do - Ltot(:) = Ltot(:) + cb%mass * cb%xb(:) .cross. cb%vb(:) + Ltot(:) = Ltot(:) + cb%mass * (cb%xb(:) .cross. cb%vb(:)) call pl%b2h(cb) oldstat = pl%status(ipl) pl%status(ipl) = INACTIVE @@ -108,28 +133,28 @@ subroutine symba_discard_conserve_mtm(pl, system, param, ipl, lescape_body) pl%status(ipl) = oldstat do i = 1, pl%nbody if (i == ipl) cycle - Lpl(:) = pl%mass(i) * pl%xb(:,i) .cross. pl%vb(:, i) + Lpl(:) = pl%mass(i) * (pl%xb(:,i) .cross. pl%vb(:, i)) Ltot(:) = Ltot(:) - Lpl(:) end do - Ltot(:) = Ltot(:) - cb%mass * cb%xb(:) .cross. cb%vb(:) - system%Lescape(:) = system%Lescape(:) + Ltot(:) - if (param%lrotation) system%Lescape(:) = system%Lescape + pl%mass(ipl) * pl%radius(ipl)**2 * pl%Ip(3, ipl) * pl%rot(:, ipl) + Ltot(:) = Ltot(:) - cb%mass * (cb%xb(:) .cross. cb%vb(:)) + param%Lescape(:) = param%Lescape(:) + Ltot(:) + if (param%lrotation) param%Lescape(:) = param%Lescape + pl%mass(ipl) * pl%radius(ipl)**2 * pl%Ip(3, ipl) * pl%rot(:, ipl) else xcom(:) = (pl%mass(ipl) * pl%xb(:, ipl) + cb%mass * cb%xb(:)) / (cb%mass + pl%mass(ipl)) vcom(:) = (pl%mass(ipl) * pl%vb(:, ipl) + cb%mass * cb%vb(:)) / (cb%mass + pl%mass(ipl)) - Lpl(:) = (pl%xb(:,ipl) - xcom(:)) .cross. pL%vb(:,ipl) - vcom(:) + Lpl(:) = (pl%xb(:,ipl) - xcom(:)) .cross. (pL%vb(:,ipl) - vcom(:)) if (param%lrotation) Lpl(:) = pl%mass(ipl) * (Lpl(:) + pl%radius(ipl)**2 * pl%Ip(3,ipl) * pl%rot(:, ipl)) - Lcb(:) = cb%mass * (cb%xb(:) - xcom(:)) .cross. (cb%vb(:) - vcom(:)) + Lcb(:) = cb%mass * ((cb%xb(:) - xcom(:)) .cross. (cb%vb(:) - vcom(:))) ke_orbit = ke_orbit + 0.5_DP * cb%mass * dot_product(cb%vb(:), cb%vb(:)) if (param%lrotation) ke_spin = ke_spin + 0.5_DP * cb%mass * cb%radius**2 * cb%Ip(3) * dot_product(cb%rot(:), cb%rot(:)) ! Update mass of central body to be consistent with its total mass - cb%dM = cb%dM + pl%mass(ipl) + cb%dGM = cb%dGM + pl%Gmass(ipl) cb%dR = cb%dR + 1.0_DP / 3.0_DP * (pl%radius(ipl) / cb%radius)**3 - 2.0_DP / 9.0_DP * (pl%radius(ipl) / cb%radius)**6 - cb%mass = cb%M0 + cb%dM - cb%Gmass = param%GU * cb%mass + cb%Gmass = cb%GM0 + cb%dGM + cb%mass = cb%Gmass / param%GU cb%radius = cb%R0 + cb%dR param%rmin = cb%radius ! Add planet angular momentum to central body accumulator @@ -147,16 +172,15 @@ subroutine symba_discard_conserve_mtm(pl, system, param, ipl, lescape_body) ! We must do this for proper book-keeping, since we can no longer track this body's contribution to energy directly if (lescape_body) then - system%Ecollisions = system%Ecollisions + ke_orbit + ke_spin + pe - system%Euntracked = system%Euntracked - (ke_orbit + ke_spin + pe) + param%Ecollisions = param%Ecollisions + ke_orbit + ke_spin + pe + param%Euntracked = param%Euntracked - (ke_orbit + ke_spin + pe) else - system%Ecollisions = system%Ecollisions + pe - system%Euntracked = system%Euntracked - pe + param%Ecollisions = param%Ecollisions + pe + param%Euntracked = param%Euntracked - pe end if end select return - end subroutine symba_discard_conserve_mtm @@ -173,18 +197,34 @@ subroutine symba_discard_nonplpl(pl, system, param) class(symba_pl), intent(inout) :: pl !! SyMBA test particle object class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + logical, dimension(pl%nbody) :: ldiscard + integer(I4B) :: i, nstart, nend, nsub + class(symba_pl), allocatable :: plsub ! First check for collisions with the central body associate(npl => pl%nbody, cb => system%cb) if (npl == 0) return - if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or. & - (param%rmaxu >= 0.0_DP) .or. ((param%qmin >= 0.0_DP) .and. (param%qmin_coord == "BARY"))) then - call pl%h2b(cb) - end if - if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or. (param%rmaxu >= 0.0_DP)) then - call symba_discard_cb_pl(pl, system, param) - end if - if (param%qmin >= 0.0_DP .and. npl > 0) call symba_discard_peri_pl(pl, system, param) + select type(pl_discards => system%pl_discards) + class is (symba_merger) + if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or. (param%rmaxu >= 0.0_DP)) then + call symba_discard_cb_pl(pl, system, param) + end if + if (param%qmin >= 0.0_DP) call symba_discard_peri_pl(pl, system, param) + if (any(pl%ldiscard(1:npl))) then + ldiscard(1:npl) = pl%ldiscard(1:npl) + + allocate(plsub, mold=pl) + call pl%spill(plsub, ldiscard, ldestructive=.false.) + nsub = plsub%nbody + nstart = pl_discards%nbody + 1 + nend = pl_discards%nbody + nsub + call pl_discards%append(plsub, lsource_mask=[(.true., i = 1, nsub)]) + + ! Record how many bodies were subtracted in this event + pl_discards%ncomp(nstart:nend) = nsub + end if + end select end associate return @@ -246,6 +286,7 @@ subroutine symba_discard_peri_pl(pl, system, param) logical, save :: lfirst = .true. logical :: lfirst_orig integer(I4B) :: i + character(len=STRMAX) :: timestr, idstr lfirst_orig = pl%lfirst @@ -262,7 +303,10 @@ subroutine symba_discard_peri_pl(pl, system, param) pl%ldiscard(i) = .true. pl%lcollision(i) = .false. pl%status(i) = DISCARDED_PERI - write(*, *) "Particle ", pl%id(i), " perihelion distance too small at t = ", param%t + write(timestr, *) param%t + write(idstr, *) pl%id(i) + write(*, *) trim(adjustl(pl%info(i)%name)) // " (" // trim(adjustl(idstr)) // ") perihelion distance too small at t = " // trim(adjustl(timestr)) + call pl%info(i)%set_value(status="DISCARDED_PERI", discard_time=param%t, discard_xh=pl%xh(:,i), discard_vh=pl%vh(:,i), discard_body_id=system%cb%id) end if end if end if @@ -277,8 +321,7 @@ end subroutine symba_discard_peri_pl module subroutine symba_discard_pl(self, system, param) !! author: David A. Minton !! - !! Call the various flavors of discards for massive bodies in SyMBA runs, including discards due to colling with the central body, - !! escaping the system, or colliding with each other. + !! Call the various flavors of discards for massive bodies in SyMBA runs, including discards due to colliding with the central body or escaping the system implicit none ! Arguments class(symba_pl), intent(inout) :: self !! SyMBA test particle object @@ -291,36 +334,31 @@ module subroutine symba_discard_pl(self, system, param) class is (symba_nbody_system) select type(param) class is (symba_parameters) - associate(pl => self, plplenc_list => system%plplenc_list) - call pl%h2b(system%cb) + associate(pl => self, plplenc_list => system%plplenc_list, plplcollision_list => system%plplcollision_list) + call pl%vb2vh(system%cb) + call pl%xh2xb(system%cb) + call plplenc_list%write(pl, pl, param) - ! First deal with the non pl-pl collisions call symba_discard_nonplpl(self, system, param) - ! Scrub the pl-pl encounter list of any encounters that did not lead to a collision - call plplenc_list%scrub_non_collision(system, param) + if (.not.any(pl%ldiscard(:))) return - if ((plplenc_list%nenc > 0) .and. any(pl%lcollision(:))) then - write(*, *) "Collision between massive bodies detected at time t = ",param%t - if (param%lfragmentation) then - call plplenc_list%resolve_fragmentations(system, param) - else - call plplenc_list%resolve_mergers(system, param) - end if + if (param%lenergy) then + call system%get_energy_and_momentum(param) + Eorbit_before = system%te end if - if (any(pl%ldiscard(:))) then - if (param%lenergy) then - call system%get_energy_and_momentum(param) - Eorbit_before = system%te - end if - call symba_discard_nonplpl_conservation(self, system, param) - call pl%rearray(system, param) - if (param%lenergy) then - call system%get_energy_and_momentum(param) - Eorbit_after = system%te - system%Ecollisions = Eorbit_after - Eorbit_before - end if + call symba_discard_nonplpl_conservation(self, system, param) + + ! Save the add/discard information to file + call system%write_discard(param) + + call pl%rearray(system, param) + + if (param%lenergy) then + call system%get_energy_and_momentum(param) + Eorbit_after = system%te + param%Ecollisions = param%Ecollisions + (Eorbit_after - Eorbit_before) end if end associate diff --git a/src/symba/symba_drift.f90 b/src/symba/symba_drift.f90 index c4efee05f..e3bbc3660 100644 --- a/src/symba/symba_drift.f90 +++ b/src/symba/symba_drift.f90 @@ -14,13 +14,14 @@ module subroutine symba_drift_pl(self, system, param, dt) real(DP), intent(in) :: dt !! Stepsize if (self%nbody == 0) return - - select type(system) - class is (symba_nbody_system) - self%lmask(:) = self%status(:) /= INACTIVE .and. self%levelg(:) == system%irec - call helio_drift_body(self, system, param, dt) - self%lmask(:) = self%status(:) /= INACTIVE - end select + associate(pl => self, npl => self%nbody) + select type(system) + class is (symba_nbody_system) + pl%lmask(1:npl) = pl%status(1:npl) /= INACTIVE .and. pl%levelg(1:npl) == system%irec + call helio_drift_body(pl, system, param, dt) + pl%lmask(1:npl) = pl%status(1:npl) /= INACTIVE + end select + end associate return end subroutine symba_drift_pl @@ -38,13 +39,14 @@ module subroutine symba_drift_tp(self, system, param, dt) real(DP), intent(in) :: dt !! Stepsize if (self%nbody == 0) return - - select type(system) - class is (symba_nbody_system) - self%lmask(:) = self%status(:) /= INACTIVE .and. self%levelg(:) == system%irec - call helio_drift_body(self, system, param, dt) - self%lmask(:) = self%status(:) /= INACTIVE - end select + associate (tp => self, ntp => self%nbody) + select type(system) + class is (symba_nbody_system) + tp%lmask(1:ntp) = tp%status(1:ntp) /= INACTIVE .and. tp%levelg(1:ntp) == system%irec + call helio_drift_body(tp, system, param, dt) + tp%lmask(1:ntp) = tp%status(1:ntp) /= INACTIVE + end select + end associate return end subroutine symba_drift_tp diff --git a/src/symba/symba_encounter_check.f90 b/src/symba/symba_encounter_check.f90 index 808ee2347..6f6010047 100644 --- a/src/symba/symba_encounter_check.f90 +++ b/src/symba/symba_encounter_check.f90 @@ -2,6 +2,46 @@ use swiftest contains + subroutine symba_encounter_check_all(nplplm, k_plpl, x, v, rhill, dt, irec, lencounter, loc_lvdotr) + !! author: David A. Minton + !! + !! Check for encounters between massive bodies. Split off from the main subroutine for performance + implicit none + integer(I8B), intent(in) :: nplplm + integer(I4B), dimension(:,:), intent(in) :: k_plpl + real(DP), dimension(:,:), intent(in) :: x, v + real(DP), dimension(:), intent(in) :: rhill + real(DP), intent(in) :: dt + integer(I4B), intent(in) :: irec + logical, dimension(:), intent(out) :: lencounter, loc_lvdotr + ! Internals + integer(I8B) :: k + integer(I4B) :: i, j + real(DP) :: xr, yr, zr, vxr, vyr, vzr, rhill1, rhill2 + + !$omp parallel do default(private)& + !$omp shared(nplplm, k_plpl, x, v, rhill, dt, irec, lencounter, loc_lvdotr) + do k = 1_I8B, nplplm + i = k_plpl(1, k) + j = k_plpl(2, k) + xr = x(1, j) - x(1, i) + yr = x(2, j) - x(2, i) + zr = x(3, j) - x(3, i) + vxr = v(1, j) - v(1, i) + vyr = v(2, j) - v(2, i) + vzr = v(3, j) - v(3, i) + rhill1 = rhill(i) + rhill2 = rhill(j) + lencounter(k) = .false. + loc_lvdotr(k) = .false. + call symba_encounter_check_one(xr, yr, zr, vxr, vyr, vzr, rhill1, rhill2, dt, irec, lencounter(k), loc_lvdotr(k)) + end do + !$omp end parallel do + + return + end subroutine symba_encounter_check_all + + module function symba_encounter_check_pl(self, system, dt, irec) result(lany_encounter) !! author: David A. Minton !! @@ -16,38 +56,47 @@ module function symba_encounter_check_pl(self, system, dt, irec) result(lany_enc ! Result logical :: lany_encounter !! Returns true if there is at least one close encounter ! Internals - integer(I8B) :: k - integer(I4B) :: nenc - real(DP), dimension(NDIM) :: xr, vr - logical, dimension(:), allocatable :: lencounter, loc_lvdotr + integer(I8B) :: k, nplplm + integer(I4B) :: i, j, nenc + logical, dimension(:), allocatable :: lencounter, loc_lvdotr if (self%nbody == 0) return - associate(pl => self, npl => self%nbody, nplpl => self%nplpl) - allocate(lencounter(nplpl), loc_lvdotr(nplpl)) - lencounter(:) = .false. - - do k = 1, nplpl - associate(i => pl%k_plpl(1, k), j => pl%k_plpl(2, k)) - xr(:) = pl%xh(:, j) - pl%xh(:, i) - vr(:) = pl%vh(:, j) - pl%vh(:, i) - call symba_encounter_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%rhill(i), pl%rhill(j), dt, irec, lencounter(k), loc_lvdotr(k)) - end associate - end do + associate(pl => self) + nplplm = pl%nplplm + allocate(lencounter(nplplm)) + allocate(loc_lvdotr(nplplm)) + + call symba_encounter_check_all(nplplm, pl%k_plpl, pl%xh, pl%vh, pl%rhill, dt, irec, lencounter, loc_lvdotr) + !$omp parallel workshare nenc = count(lencounter(:)) + !$omp end parallel workshare + lany_encounter = nenc > 0 if (lany_encounter) then associate(plplenc_list => system%plplenc_list) call plplenc_list%resize(nenc) - plplenc_list%lvdotr(1:nenc) = pack(loc_lvdotr(:), lencounter(:)) - plplenc_list%index1(1:nenc) = pack(pl%k_plpl(1,:), lencounter(:)) - plplenc_list%index2(1:nenc) = pack(pl%k_plpl(2,:), lencounter(:)) + plplenc_list%lvdotr(1:nenc) = pack(loc_lvdotr(1:nplplm), lencounter(1:nplplm)) + plplenc_list%kidx(1:nenc) = pack([(k, k = 1_I8B, nplplm)], lencounter(1:nplplm)) + deallocate(lencounter, loc_lvdotr) + plplenc_list%index1(1:nenc) = pl%k_plpl(1,plplenc_list%kidx(1:nenc)) + plplenc_list%index2(1:nenc) = pl%k_plpl(2,plplenc_list%kidx(1:nenc)) + plplenc_list%id1(1:nenc) = pl%id(plplenc_list%index1(1:nenc)) + plplenc_list%id2(1:nenc) = pl%id(plplenc_list%index2(1:nenc)) do k = 1, nenc + i = plplenc_list%index1(k) + j = plplenc_list%index2(k) plplenc_list%status(k) = ACTIVE plplenc_list%level(k) = irec - pl%lencounter(plplenc_list%index1(k)) = .true. - pl%lencounter(plplenc_list%index2(k)) = .true. + pl%lencounter(i) = .true. + pl%lencounter(j) = .true. + pl%levelg(i) = irec + pl%levelm(i) = irec + pl%levelg(j) = irec + pl%levelm(j) = irec + pl%nplenc(i) = pl%nplenc(i) + 1 + pl%nplenc(j) = pl%nplenc(j) + 1 end do end associate end if @@ -56,7 +105,7 @@ module function symba_encounter_check_pl(self, system, dt, irec) result(lany_enc end function symba_encounter_check_pl - module function symba_encounter_check_pltpenc(self, system, dt, irec) result(lany_encounter) + module function symba_encounter_check(self, system, dt, irec) result(lany_encounter) !! author: David A. Minton !! !! Check for an encounter between test particles and massive bodies in the pltpenc list. @@ -65,13 +114,13 @@ module function symba_encounter_check_pltpenc(self, system, dt, irec) result(lan !! Adapted from portions of David E. Kaufmann's Swifter routine: symba_step_recur.f90 implicit none ! Arguments - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-pl encounter list object + class(symba_encounter), intent(inout) :: self !! SyMBA pl-pl encounter list object class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object real(DP), intent(in) :: dt !! step size integer(I4B), intent(in) :: irec !! Current recursion level logical :: lany_encounter !! Returns true if there is at least one close encounter ! Internals - integer(I4B) :: k + integer(I4B) :: i, j,k real(DP), dimension(NDIM) :: xr, vr logical :: lencounter, isplpl real(DP) :: rlim2, rji2 @@ -94,45 +143,45 @@ module function symba_encounter_check_pltpenc(self, system, dt, irec) result(lan allocate(lencmask(self%nenc)) lencmask(:) = (self%status(1:self%nenc) == ACTIVE) .and. (self%level(1:self%nenc) == irec - 1) if (.not.any(lencmask(:))) return - associate(ind1 => self%index1, ind2 => self%index2) - do concurrent(k = 1:self%nenc, lencmask(k)) + do concurrent(k = 1:self%nenc, lencmask(k)) + i = self%index1(k) + j = self%index2(k) + if (isplpl) then + xr(:) = pl%xh(:,j) - pl%xh(:,i) + vr(:) = pl%vb(:,j) - pl%vb(:,i) + call symba_encounter_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%rhill(i), pl%rhill(j), dt, irec, lencounter, self%lvdotr(k)) + else + xr(:) = tp%xh(:,j) - pl%xh(:,i) + vr(:) = tp%vb(:,j) - pl%vb(:,i) + call symba_encounter_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%rhill(i), 0.0_DP, dt, irec, lencounter, self%lvdotr(k)) + end if + if (lencounter) then if (isplpl) then - xr(:) = pl%xh(:,ind2(k)) - pl%xh(:,ind1(k)) - vr(:) = pl%vb(:,ind2(k)) - pl%vb(:,ind1(k)) - call symba_encounter_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%rhill(ind1(k)), pl%rhill(ind2(k)), dt, irec, lencounter, self%lvdotr(k)) + rlim2 = (pl%radius(i) + pl%radius(j))**2 else - xr(:) = tp%xh(:,ind2(k)) - pl%xh(:,ind1(k)) - vr(:) = tp%vb(:,ind2(k)) - pl%vb(:,ind1(k)) - call symba_encounter_check_one(xr(1), xr(2), xr(3), vr(1), vr(2), vr(3), pl%rhill(ind1(k)), 0.0_DP, dt, irec, lencounter, self%lvdotr(k)) + rlim2 = (pl%radius(i))**2 end if - if (lencounter) then + rji2 = dot_product(xr(:), xr(:))! Check to see if these are physically overlapping bodies first, which we should ignore + if (rji2 > rlim2) then + lany_encounter = .true. + pl%levelg(i) = irec + pl%levelm(i) = MAX(irec, pl%levelm(i)) if (isplpl) then - rlim2 = (pl%radius(ind1(k)) + pl%radius(ind2(k)))**2 + pl%levelg(j) = irec + pl%levelm(j) = MAX(irec, pl%levelm(j)) else - rlim2 = (pl%radius(ind1(k)))**2 + tp%levelg(j) = irec + tp%levelm(j) = MAX(irec, tp%levelm(j)) end if - rji2 = dot_product(xr(:), xr(:))! Check to see if these are physically overlapping bodies first, which we should ignore - if (rji2 > rlim2) then - lany_encounter = .true. - pl%levelg(ind1(k)) = irec - pl%levelm(ind1(k)) = MAX(irec, pl%levelm(ind1(k))) - if (isplpl) then - pl%levelg(ind2(k)) = irec - pl%levelm(ind2(k)) = MAX(irec, pl%levelm(ind2(k))) - else - tp%levelg(ind2(k)) = irec - tp%levelm(ind2(k)) = MAX(irec, tp%levelm(ind2(k))) - end if - self%level(k) = irec - end if - end if - end do - end associate + self%level(k) = irec + end if + end if + end do end select end select return - end function symba_encounter_check_pltpenc + end function symba_encounter_check module function symba_encounter_check_tp(self, system, dt, irec) result(lany_encounter) @@ -150,7 +199,7 @@ module function symba_encounter_check_tp(self, system, dt, irec) result(lany_enc logical :: lany_encounter !! Returns true if there is at least one close encounter ! Internals real(DP) :: r2crit, vdotr, r2, v2, tmin, r2min, term2 - integer(I4B) :: i, j, k,nenc + integer(I4B) :: i, j, k,nenc, plind, tpind real(DP), dimension(NDIM) :: xr, vr logical, dimension(:,:), allocatable :: lencounter, loc_lvdotr @@ -175,14 +224,24 @@ module function symba_encounter_check_tp(self, system, dt, irec) result(lany_enc call pltpenc_list%resize(nenc) pltpenc_list%status(1:nenc) = ACTIVE pltpenc_list%level(1:nenc) = irec - pltpenc_list%lvdotr(1:nenc) = pack(loc_lvdotr(:,:), lencounter(:,:)) - pltpenc_list%index1(1:nenc) = pack(spread([(i, i = 1, npl)], dim=1, ncopies=ntp), lencounter(:,:)) - pltpenc_list%index2(1:nenc) = pack(spread([(i, i = 1, ntp)], dim=2, ncopies=npl), lencounter(:,:)) + pltpenc_list%lvdotr(1:nenc) = pack(loc_lvdotr(1:ntp, 1:npl), lencounter(1:ntp, 1:npl)) + pltpenc_list%index1(1:nenc) = pack(spread([(i, i = 1, npl)], dim=1, ncopies=ntp), lencounter(1:ntp, 1:npl)) + pltpenc_list%index2(1:nenc) = pack(spread([(i, i = 1, ntp)], dim=2, ncopies=npl), lencounter(1:ntp, 1:npl)) + pltpenc_list%id1(1:nenc) = pl%id(pltpenc_list%index1(1:nenc)) + pltpenc_list%id2(1:nenc) = tp%id(pltpenc_list%index2(1:nenc)) select type(pl) class is (symba_pl) - pl%lencounter(:) = .false. + pl%lencounter(1:npl) = .false. do k = 1, nenc - pl%lencounter(pltpenc_list%index1(k)) = .true. + plind = pltpenc_list%index1(k) + tpind = pltpenc_list%index2(k) + pl%lencounter(plind) = .true. + pl%levelg(plind) = irec + pl%levelm(plind) = irec + tp%levelg(tpind) = irec + tp%levelm(tpind) = irec + pl%ntpenc(plind) = pl%ntpenc(plind) + 1 + tp%nplenc(tpind) = tp%nplenc(tpind) + 1 end do end select end associate diff --git a/src/symba/symba_fragmentation.f90 b/src/symba/symba_fragmentation.f90 deleted file mode 100644 index b36c54e9a..000000000 --- a/src/symba/symba_fragmentation.f90 +++ /dev/null @@ -1,470 +0,0 @@ -submodule (symba_classes) s_symba_fragmentation - use swiftest - - integer(I4B), parameter :: NFRAG_DISRUPT = 12 - integer(I4B), parameter :: NFRAG_SUPERCAT = 20 -contains - - module function symba_fragmentation_casedisruption(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Create the fragments resulting from a non-catastrophic disruption collision - !! - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collision - ! Result - integer(I4B) :: status !! Status flag assigned to this outcome - ! Internals - integer(I4B) :: i, istart, nfrag, ibiggest, nfamily, nstart, nend - real(DP) :: mtot, avg_dens - real(DP), dimension(NDIM) :: xcom, vcom, Ip_new - real(DP), dimension(2) :: vol - real(DP), dimension(:, :), allocatable :: vb_frag, xb_frag, rot_frag, Ip_frag - real(DP), dimension(:), allocatable :: m_frag, rad_frag - integer(I4B), dimension(:), allocatable :: id_frag - logical :: lfailure - - ! Collisional fragments will be uniformly distributed around the pre-impact barycenter - nfrag = NFRAG_DISRUPT - allocate(m_frag(nfrag)) - allocate(rad_frag(nfrag)) - allocate(xb_frag(NDIM, nfrag)) - allocate(vb_frag(NDIM, nfrag)) - allocate(rot_frag(NDIM, nfrag)) - allocate(Ip_frag(NDIM, nfrag)) - allocate(id_frag(nfrag)) - - mtot = sum(mass(:)) - xcom(:) = (mass(1) * x(:,1) + mass(2) * x(:,2)) / mtot - vcom(:) = (mass(1) * v(:,1) + mass(2) * v(:,2)) / mtot - - ! Get mass weighted mean of Ip and average density - Ip_new(:) = (mass(1) * Ip(:,1) + mass(2) * Ip(:,2)) / mtot - vol(:) = 4._DP / 3._DP * PI * radius(:)**3 - avg_dens = mtot / sum(vol(:)) - - ! Distribute the mass among fragments, with a branch to check for the size of the second largest fragment - m_frag(1) = mass_res(1) - if (mass_res(2) > mass_res(1) / 3._DP) then - m_frag(2) = mass_res(2) - istart = 3 - else - istart = 2 - end if - ! Distribute remaining mass among the remaining bodies - do i = istart, nfrag - m_frag(i) = (mtot - sum(m_frag(1:istart - 1))) / (nfrag - istart + 1) - end do - - ! Distribute any residual mass if there is any and set the radius - m_frag(nfrag) = m_frag(nfrag) + (mtot - sum(m_frag(:))) - rad_frag(:) = (3 * m_frag(:) / (4 * PI * avg_dens))**(1.0_DP / 3.0_DP) - id_frag(:) = [(i, i = system%maxid + 1, system%maxid + nfrag)] - - do i = 1, nfrag - Ip_frag(:, i) = Ip_new(:) - end do - - call fragmentation_initialize(system, param, family, x, v, L_spin, Ip, mass, radius, & - nfrag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, Qloss, lfailure) - - if (lfailure) then - write(*,*) 'No fragment solution found, so treat as a pure hit-and-run' - status = ACTIVE - nfrag = 0 - else - ! Populate the list of new bodies - write(*,'("Generating ",I2.0," fragments")') nfrag - status = DISRUPTION - call symba_fragmentation_mergeaddsub(system, param, family, id_frag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, status) - end if - - return - end function symba_fragmentation_casedisruption - - - module function symba_fragmentation_casehitandrun(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Create the fragments resulting from a non-catastrophic hit-and-run collision - !! - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collision - ! Result - integer(I4B) :: status !! Status flag assigned to this outcome - ! Internals - integer(I4B) :: i, nfrag, jproj, jtarg, idstart, ibiggest, nfamily - real(DP) :: mtot, avg_dens - real(DP), dimension(NDIM) :: xcom, vcom - real(DP), dimension(2) :: vol - real(DP), dimension(:, :), allocatable :: vb_frag, xb_frag, rot_frag, Ip_frag - real(DP), dimension(:), allocatable :: m_frag, rad_frag - integer(I4B), dimension(:), allocatable :: id_frag - logical :: lpure - logical, dimension(system%pl%nbody) :: lmask - - mtot = sum(mass(:)) - xcom(:) = (mass(1) * x(:,1) + mass(2) * x(:,2)) / mtot - vcom(:) = (mass(1) * v(:,1) + mass(2) * v(:,2)) / mtot - lpure = .false. - - ! The largest body will stay untouched - if (mass(1) > mass(2)) then - jtarg = 1 - jproj = 2 - else - jtarg = 2 - jproj = 1 - end if - - if (mass_res(2) > 0.9_DP * mass(jproj)) then ! Pure hit and run, so we'll just keep the two bodies untouched - write(*,*) 'Pure hit and run. No new fragments generated.' - nfrag = 0 - lpure = .true. - else ! Imperfect hit and run, so we'll keep the largest body and destroy the other - nfrag = NFRAG_DISRUPT - 1 - lpure = .false. - allocate(m_frag(nfrag)) - allocate(id_frag(nfrag)) - allocate(rad_frag(nfrag)) - allocate(xb_frag(NDIM, nfrag)) - allocate(vb_frag(NDIM, nfrag)) - allocate(rot_frag(NDIM, nfrag)) - allocate(Ip_frag(NDIM, nfrag)) - m_frag(1) = mass(jtarg) - ibiggest = maxloc(system%pl%Gmass(family(:)), dim=1) - id_frag(1) = system%pl%id(ibiggest) - rad_frag(1) = radius(jtarg) - xb_frag(:, 1) = x(:, jtarg) - vb_frag(:, 1) = v(:, jtarg) - Ip_frag(:,1) = Ip(:, jtarg) - - ! Get mass weighted mean of Ip and average density - vol(:) = 4._DP / 3._DP * pi * radius(:)**3 - avg_dens = mass(jproj) / vol(jproj) - m_frag(2:nfrag) = (mtot - m_frag(1)) / (nfrag - 1) - rad_frag(2:nfrag) = (3 * m_frag(2:nfrag) / (4 * PI * avg_dens))**(1.0_DP / 3.0_DP) - m_frag(nfrag) = m_frag(nfrag) + (mtot - sum(m_frag(:))) - id_frag(2:nfrag) = [(i, i = system%maxid + 1, system%maxid + nfrag - 1)] - - do i = 1, nfrag - Ip_frag(:, i) = Ip(:, jproj) - end do - - ! Put the fragments on the circle surrounding the center of mass of the system - call fragmentation_initialize(system, param, family, x, v, L_spin, Ip, mass, radius, & - nfrag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, Qloss, lpure) - if (lpure) then - write(*,*) 'Should have been a pure hit and run instead' - nfrag = 0 - else - write(*,'("Generating ",I2.0," fragments")') nfrag - end if - end if - if (lpure) then - status = ACTIVE - else - status = HIT_AND_RUN - call symba_fragmentation_mergeaddsub(system, param, family, id_frag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, status) - end if - - return - end function symba_fragmentation_casehitandrun - - - module function symba_fragmentation_casemerge(system, param, family, x, v, mass, radius, L_spin, Ip) result(status) - !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Merge planets. - !! - !! Adapted from David E. Kaufmann's Swifter routines symba_merge_pl.f90 and symba_discard_merge_pl.f90 - !! - !! Adapted from Hal Levison's Swift routines symba5_merge.f and discard_mass_merge.f - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(in) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(in) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - ! Result - integer(I4B) :: status !! Status flag assigned to this outcome - ! Internals - integer(I4B) :: i, j, ibiggest, nfamily - real(DP) :: volume_new, pe - real(DP), dimension(NDIM) :: xc, vc, xcrossv - real(DP), dimension(2) :: vol - real(DP), dimension(NDIM) :: L_orb_old, L_spin_old - real(DP), dimension(NDIM) :: L_spin_new - logical, dimension(system%pl%nbody) :: lmask - real(DP), dimension(NDIM, 1) :: vb_frag, xb_frag, rot_frag, Ip_frag - real(DP), dimension(1) :: m_frag, rad_frag - integer(I4B), dimension(1) :: id_frag - - select type(pl => system%pl) - class is (symba_pl) - write(*, '("Merging bodies ",99(I8,",",:))') pl%id(family(:)) - - ibiggest = maxloc(pl%Gmass(family(:)), dim=1) - id_frag(1) = pl%id(family(ibiggest)) - - m_frag(1) = sum(mass(:)) - - ! Merged body is created at the barycenter of the original bodies - xb_frag(:,1) = (mass(1) * x(:,1) + mass(2) * x(:,2)) / m_frag(1) - vb_frag(:,1) = (mass(1) * v(:,1) + mass(2) * v(:,2)) / m_frag(1) - - ! Get mass weighted mean of Ip and - vol(:) = 4._DP / 3._DP * PI * radius(:)**3 - volume_new = sum(vol(:)) - rad_frag(1) = (3 * volume_new / (4 * PI))**(1._DP / 3._DP) - - L_orb_old(:) = 0.0_DP - - ! Compute orbital angular momentum of pre-impact system - do i = 1, 2 - xc(:) = x(:, i) - xb_frag(:,1) - vc(:) = v(:, i) - vb_frag(:,1) - xcrossv(:) = xc(:) .cross. vc(:) - L_orb_old(:) = L_orb_old(:) + mass(i) * xcrossv(:) - end do - - if (param%lrotation) then - Ip_frag(:,1) = (mass(1) * Ip(:,1) + mass(2) * Ip(:,2)) / m_frag(1) - L_spin_old(:) = L_spin(:,1) + L_spin(:,2) - - ! Conserve angular momentum by putting pre-impact orbital momentum into spin of the new body - L_spin_new(:) = L_orb_old(:) + L_spin_old(:) - - ! Assume prinicpal axis rotation on 3rd Ip axis - rot_frag(:,1) = L_spin_new(:) / (Ip_frag(3,1) * m_frag(1) * rad_frag(1)**2) - else ! If spin is not enabled, we will consider the lost pre-collision angular momentum as "escaped" and add it to our bookkeeping variable - system%Lescape(:) = system%Lescape(:) + L_orb_old(:) - end if - - ! Keep track of the component of potential energy due to the pre-impact family for book-keeping - nfamily = size(family(:)) - pe = 0.0_DP - do j = 1, nfamily - do i = j + 1, nfamily - pe = pe - pl%mass(i) * pl%mass(j) / norm2(pl%xb(:, i) - pl%xb(:, j)) - end do - end do - system%Ecollisions = system%Ecollisions + pe - system%Euntracked = system%Euntracked - pe - - status = MERGED - call symba_fragmentation_mergeaddsub(system, param, family, id_frag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, status) - - end select - - return - end function symba_fragmentation_casemerge - - - module function symba_fragmentation_casesupercatastrophic(system, param, family, x, v, mass, radius, L_spin, Ip, mass_res, Qloss) result(status) - !! author: Jennifer L.L. Pouplin, Carlisle A. Wishard, and David A. Minton - !! - !! Create the fragments resulting from a supercatastrophic collision - !! - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - real(DP), dimension(:,:), intent(inout) :: x, v, L_spin, Ip !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass, radius !! Input values that represent a 2-body equivalent of a possibly 2+ body collision - real(DP), dimension(:), intent(inout) :: mass_res !! The distribution of fragment mass obtained by the regime calculation - real(DP), intent(inout) :: Qloss !! Energy lost during collision - ! Result - integer(I4B) :: status !! Status flag assigned to this outcome - ! Internals - integer(I4B) :: i, nfrag, ibiggest, nfamily, nstart, nend - real(DP) :: mtot, avg_dens, min_frag_mass - real(DP), dimension(NDIM) :: xcom, vcom - real(DP), dimension(2) :: vol - real(DP), dimension(NDIM) :: Ip_new - real(DP), dimension(:, :), allocatable :: vb_frag, xb_frag, rot_frag, Ip_frag - real(DP), dimension(:), allocatable :: m_frag, rad_frag - integer(I4B), dimension(:), allocatable :: id_frag - logical :: lfailure - logical, dimension(system%pl%nbody) :: lmask - - ! Collisional fragments will be uniformly distributed around the pre-impact barycenter - nfrag = NFRAG_SUPERCAT - allocate(m_frag(nfrag)) - allocate(rad_frag(nfrag)) - allocate(id_frag(nfrag)) - allocate(xb_frag(NDIM, nfrag)) - allocate(vb_frag(NDIM, nfrag)) - allocate(rot_frag(NDIM, nfrag)) - allocate(Ip_frag(NDIM, nfrag)) - - mtot = sum(mass(:)) - xcom(:) = (mass(1) * x(:,1) + mass(2) * x(:,2)) / mtot - vcom(:) = (mass(1) * v(:,1) + mass(2) * v(:,2)) / mtot - - ! Get mass weighted mean of Ip and average density - Ip_new(:) = (mass(1) * Ip(:,1) + mass(2) * Ip(:,2)) / mtot - vol(:) = 4._DP / 3._DP * pi * radius(:)**3 - avg_dens = mtot / sum(vol(:)) - - ! If we are adding the first and largest fragment (lr), check to see if its mass is SMALLER than an equal distribution of - ! mass between all fragments. If so, we will just distribute the mass equally between the fragments - min_frag_mass = mtot / nfrag - if (mass_res(1) < min_frag_mass) then - m_frag(:) = min_frag_mass - else - m_frag(1) = mass_res(1) - m_frag(2:nfrag) = (mtot - mass_res(1)) / (nfrag - 1) - end if - ! Distribute any residual mass if there is any and set the radius - m_frag(nfrag) = m_frag(nfrag) + (mtot - sum(m_frag(:))) - rad_frag(:) = (3 * m_frag(:) / (4 * PI * avg_dens))**(1.0_DP / 3.0_DP) - id_frag(:) = [(i, i = system%maxid + 1, system%maxid + nfrag)] - - do i = 1, nfrag - Ip_frag(:, i) = Ip_new(:) - end do - - call fragmentation_initialize(system, param, family, x, v, L_spin, Ip, mass, radius, & - nfrag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, Qloss, lfailure) - - if (lfailure) then - write(*,*) 'No fragment solution found, so treat as a pure hit-and-run' - status = ACTIVE - nfrag = 0 - else - ! Populate the list of new bodies - write(*,'("Generating ",I2.0," fragments")') nfrag - status = SUPERCATASTROPHIC - call symba_fragmentation_mergeaddsub(system, param, family, id_frag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, status) - end if - - return - end function symba_fragmentation_casesupercatastrophic - - - subroutine symba_fragmentation_mergeaddsub(system, param, family, id_frag, Ip_frag, m_frag, rad_frag, xb_frag, vb_frag, rot_frag, status) - !! author: David A. Minton - !! - !! Fills the pl_discards and pl_adds with removed and added bodies - !! - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions - integer(I4B), dimension(:), intent(in) :: family !! List of indices of all bodies inovlved in the collision - integer(I4B), dimension(:), intent(in) :: id_frag !! List of fragment ids - real(DP), dimension(:), intent(in) :: m_frag, rad_frag !! Distribution of fragment mass and radii - real(DP), dimension(:,:), intent(in) :: Ip_frag !! Fragment rotational inertia vectors - real(DP), dimension(:,:), intent(in) :: xb_frag, vb_frag, rot_frag !! Fragment barycentric position, barycentric velocity, and rotation vectors - integer(I4B), intent(in) :: status !! Status flag to assign to adds - ! Internals - integer(I4B) :: i, ibiggest, nstart, nend, nfamily, nfrag - logical, dimension(system%pl%nbody) :: lmask - class(symba_pl), allocatable :: plnew - - select type(pl => system%pl) - class is (symba_pl) - select type(pl_discards => system%pl_discards) - class is (symba_merger) - associate(pl_adds => system%pl_adds, cb => system%cb) - - ! Add the family bodies to the subtraction list - nfamily = size(family(:)) - nfrag = size(m_frag(:)) - lmask(:) = .false. - lmask(family(:)) = .true. - pl%status(family(:)) = MERGED - nstart = pl_discards%nbody + 1 - nend = pl_discards%nbody + nfamily - call pl_discards%append(pl, lmask) - pl%ldiscard(family(:)) = .true. - pl%lcollision(family(:)) = .true. - - ! Record how many bodies were subtracted in this event - pl_discards%ncomp(nstart:nend) = nfamily - - ! Setup new bodies - allocate(plnew, mold=pl) - call plnew%setup(nfrag, param) - ibiggest = maxloc(pl%Gmass(family(:)), dim=1) - - plnew%id(:) = id_frag(:) - system%maxid = system%maxid + nfrag - plnew%status(:) = ACTIVE - plnew%lcollision(:) = .false. - plnew%ldiscard(:) = .false. - plnew%xb(:,:) = xb_frag(:, :) - plnew%vb(:,:) = vb_frag(:, :) - do i = 1, nfrag - plnew%xh(:,i) = xb_frag(:, i) - cb%xb(:) - plnew%vh(:,i) = vb_frag(:, i) - cb%vb(:) - end do - plnew%mass(:) = m_frag(:) - plnew%Gmass(:) = param%GU * m_frag(:) - plnew%radius(:) = rad_frag(:) - plnew%density(:) = m_frag(:) / rad_frag(:) - - select case(status) - case(DISRUPTION) - plnew%info(:)%origin_type = "Disruption" - case(SUPERCATASTROPHIC) - plnew%info(:)%origin_type = "Supercatastrophic" - case(HIT_AND_RUN) - plnew%info(:)%origin_type = "Hit and run fragment" - case(MERGED) - plnew%info(1) = pl%info(ibiggest) - end select - - if (status /= MERGED) then - plnew%info(:)%origin_time = param%t - do i = 1, nfrag - plnew%info(i)%origin_xh(:) = plnew%xh(:,i) - plnew%info(i)%origin_vh(:) = plnew%vh(:,i) - end do - end if - - if (param%lrotation) then - plnew%Ip(:,:) = Ip_frag(:,:) - plnew%rot(:,:) = rot_frag(:,:) - end if - if (param%ltides) then - plnew%Q = pl%Q(ibiggest) - plnew%k2 = pl%k2(ibiggest) - plnew%tlag = pl%tlag(ibiggest) - end if - call plnew%set_mu(cb) - pl%lmtiny(:) = pl%Gmass(:) > param%GMTINY - - ! Append the new merged body to the list and record how many we made - nstart = pl_adds%nbody + 1 - nend = pl_adds%nbody + plnew%nbody - call pl_adds%append(plnew, lsource_mask=[(.true., i=1, plnew%nbody)]) - pl_adds%ncomp(nstart:nend) = plnew%nbody - - call plnew%setup(0, param) - deallocate(plnew) - end associate - end select - end select - - return - end subroutine symba_fragmentation_mergeaddsub - -end submodule s_symba_fragmentation diff --git a/src/symba/symba_io.f90 b/src/symba/symba_io.f90 index 97e5798c2..c97904079 100644 --- a/src/symba/symba_io.f90 +++ b/src/symba/symba_io.f90 @@ -2,90 +2,6 @@ use swiftest contains - module subroutine symba_io_dump_particle_info(system, param, lincludecb, tpidx, plidx) - !! author: David A. Minton - !! - !! Dumps the particle information data to a file. - !! Pass a list of array indices for test particles (tpidx) and/or massive bodies (plidx) to append - implicit none - ! Arguments - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA extensions - logical, optional, intent(in) :: lincludecb !! Set to true to include the central body (default is false) - integer(I4B), dimension(:), optional, intent(in) :: tpidx !! Array of test particle indices to append to the particle file - integer(I4B), dimension(:), optional, intent(in) :: plidx !! Array of massive body indices to append to the particle file - ! Internals - logical, save :: lfirst = .true. - integer(I4B), parameter :: LUN = 22 - integer(I4B) :: i, ierr - - if (lfirst) then - select case(param%out_stat) - case('APPEND') - open(unit = LUN, file = param%particle_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) - case('NEW', 'UNKNOWN', 'REPLACE') - open(unit = LUN, file = param%particle_out, status = param%out_stat, form = 'UNFORMATTED', iostat = ierr) - case default - write(*,*) 'Invalid status code',trim(adjustl(param%out_stat)) - call util_exit(FAILURE) - end select - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " particle output file already exists or cannot be accessed" - call util_exit(FAILURE) - end if - - lfirst = .false. - else - open(unit = LUN, file = param%particle_out, status = 'OLD', position = 'APPEND', form = 'UNFORMATTED', iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " unable to open binary output file for APPEND" - call util_exit(FAILURE) - end if - end if - - if (present(lincludecb)) then - if (lincludecb) then - select type(cb => system%cb) - class is (symba_cb) - write(LUN) cb%id - write(LUN) cb%info - end select - end if - end if - - if (present(plidx) .and. (system%pl%nbody > 0)) then - select type(pl => system%pl) - class is (symba_pl) - do i = 1, size(plidx) - write(LUN) pl%id(plidx(i)) - write(LUN) pl%info(plidx(i)) - end do - end select - end if - - if (present(tpidx) .and. (system%tp%nbody > 0)) then - select type(tp => system%tp) - class is (symba_tp) - do i = 1, size(tpidx) - write(LUN) tp%id(tpidx(i)) - write(LUN) tp%info(tpidx(i)) - end do - end select - end if - - close(unit = LUN, iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " unable to close particle output file" - call util_exit(FAILURE) - end if - - return - end subroutine symba_io_dump_particle_info - - module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, iomsg) !! author: The Purdue Swiftest Team - David A. Minton, Carlisle A. Wishard, Jennifer L.L. Pouplin, and Jacob R. Elliott !! @@ -106,9 +22,9 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms integer(I4B) :: ilength, ifirst, ilast !! Variables used to parse input file character(STRMAX) :: line !! Line of the input file character (len=:), allocatable :: line_trim,param_name, param_value !! Strings used to parse the param file - integer(I4B) :: nseeds, nseeds_from_file, i - logical :: seed_set = .false. !! Is the random seed set in the input file? - character(len=*),parameter :: linefmt = '(A)' + integer(I4B) :: nseeds, nseeds_from_file, i + logical :: seed_set = .false. !! Is the random seed set in the input file? + character(len=*),parameter :: linefmt = '(A)' associate(param => self) call io_param_reader(param, unit, iotype, v_list, iostat, iomsg) @@ -118,7 +34,7 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms allocate(param%seed(nseeds)) rewind(unit) do - read(unit = unit, fmt = linefmt, iostat = iostat, end = 1) line + read(unit = unit, fmt = linefmt, iostat = iostat, end = 1, err = 667, iomsg = iomsg) line line_trim = trim(adjustl(line)) ilength = len(line_trim) if ((ilength /= 0)) then @@ -130,13 +46,13 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms ifirst = ilast + 1 param_value = io_get_token(line_trim, ifirst, ilast, iostat) select case (param_name) - case ("PARTICLE_OUT") - param%particle_out = param_value case ("FRAGMENTATION") call io_toupper(param_value) if (param_value == "YES" .or. param_value == "T") self%lfragmentation = .true. case ("GMTINY") - read(param_value, *) param%Gmtiny + read(param_value, *) param%GMTINY + case ("MIN_GMFRAG") + read(param_value, *) param%min_GMfrag case("SEED") read(param_value, *) nseeds_from_file ! Because the number of seeds can vary between compilers/systems, we need to make sure we can handle cases in which the input file has a different @@ -147,13 +63,13 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms deallocate(param%seed) allocate(param%seed(nseeds)) do i = 1, nseeds - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) read(param_value, *) param%seed(i) end do else ! Seed array in file is too small do i = 1, nseeds_from_file - ifirst = ilast + 1 + ifirst = ilast + 2 param_value = io_get_token(line, ifirst, ilast, iostat) read(param_value, *) param%seed(i) end do @@ -165,6 +81,14 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms end do 1 continue + if (self%GMTINY < 0.0_DP) then + write(iomsg,*) "GMTINY invalid or not set: ", self%GMTINY + iostat = -1 + return + else + write(*,*) "GMTINY = ", self%GMTINY + end if + write(*,*) "FRAGMENTATION = ", param%lfragmentation if (param%lfragmentation) then if (seed_set) then @@ -173,14 +97,8 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms call random_seed(get = param%seed) end if write(*,*) "SEED: N,VAL = ",size(param%seed), param%seed(:) - end if - - if (self%Gmtiny < 0.0_DP) then - write(iomsg,*) "GMTINY invalid or not set: ", self%Gmtiny - iostat = -1 - return - else - write(*,*) "GMTINY = ", self%Gmtiny + if (param%min_GMfrag < 0.0_DP) param%min_GMfrag = param%GMTINY + write(*,*) "MIN_GMFRAG = ", self%min_GMfrag end if if (.not.self%lclose) then @@ -188,10 +106,13 @@ module subroutine symba_io_param_reader(self, unit, iotype, v_list, iostat, ioms iostat = -1 return end if + ! All reporting of collision information in SyMBA (including mergers) is now recorded in the Fraggle logfile + call fraggle_io_log_start(param) end associate iostat = 0 + 667 continue return end subroutine symba_io_param_reader @@ -217,36 +138,37 @@ module subroutine symba_io_param_writer(self, unit, iotype, v_list, iostat, ioms character(*),parameter :: Rfmt = '(ES25.17)' !! Format label for real values character(*),parameter :: Rarrfmt = '(3(ES25.17,1X))' !! Format label for real values character(*),parameter :: Lfmt = '(L1)' !! Format label for logical values - character(len=*), parameter :: Afmt = '(A25,1X,64(:,A25,1X))' - character(256) :: param_name, param_value + character(len=NAMELEN) :: param_name + character(len=STRMAX) :: param_value type character_array character(25) :: value end type character_array type(character_array), dimension(:), allocatable :: param_array - integer(I4B) :: i + integer(I4B) :: i, nstr associate(param => self) call io_param_writer(param, unit, iotype, v_list, iostat, iomsg) ! Special handling is required for writing the random number seed array as its size is not known until runtime ! For the "SEED" parameter line, the first value will be the size of the seed array and the rest will be the seed array elements - write(param_name, Afmt) "PARTICLE_OUT"; write(param_value, Afmt) trim(adjustl(param%particle_out)); write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "GMTINY"; write(param_value, Rfmt) param%Gmtiny; write(unit, Afmt) adjustl(param_name), adjustl(param_value) - write(param_name, Afmt) "FRAGMENTATION"; write(param_value, Lfmt) param%lfragmentation; write(unit, Afmt) adjustl(param_name), adjustl(param_value) + write(param_name, *) "GMTINY"; write(param_value, Rfmt) param%GMTINY; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "MIN_GMFRAG"; write(param_value, Rfmt) param%min_GMfrag; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) + write(param_name, *) "FRAGMENTATION"; write(param_value, Lfmt) param%lfragmentation; write(unit, *, err = 667, iomsg = iomsg) adjustl(param_name) // trim(adjustl(param_value)) if (param%lfragmentation) then - write(param_name, Afmt) "SEED" + write(param_name, *) "SEED" if (allocated(param_array)) deallocate(param_array) allocate(param_array(0:size(param%seed))) write(param_array(0)%value, Ifmt) size(param%seed) do i = 1, size(param%seed) write(param_array(i)%value, Ifmt) param%seed(i) end do - write(unit, Afmt, advance='no') adjustl(param_name), adjustl(param_array(0)%value) - do i = 1, size(param%seed) + write(unit, '(" ",A32)', advance='no', err = 667, iomsg = iomsg) adjustl(param_name) + do i = 0, size(param%seed) + nstr = len(trim(adjustl(param_array(i)%value))) if (i < size(param%seed)) then - write(unit, Afmt, advance='no') adjustl(param_array(i)%value) + write(unit, '(A12)', advance='no', err = 667, iomsg = iomsg) trim(adjustl(param_array(i)%value)) // " " else - write(unit, Afmt) adjustl(param_array(i)%value) + write(unit, '(A12)', err = 667, iomsg = iomsg) trim(adjustl(param_array(i)%value)) end if end do end if @@ -255,86 +177,18 @@ module subroutine symba_io_param_writer(self, unit, iotype, v_list, iostat, ioms end associate return + 667 continue + write(*,*) "Error writing parameter file for SyMBA: " // trim(adjustl(iomsg)) end subroutine symba_io_param_writer - module subroutine symba_io_read_particle(system, param) - !! author: David A. Minton - !! - !! Reads an old particle information file for a restartd run - implicit none - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system file - class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA extensions - - ! Internals - integer(I4B), parameter :: LUN = 22 - integer(I4B) :: i, ierr, id, idx - logical :: lmatch - type(symba_particle_info) :: tmpinfo - - open(unit = LUN, file = param%particle_out, status = 'OLD', form = 'UNFORMATTED', iostat = ierr) - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " unable to open binary particle file for reading" - call util_exit(FAILURE) - end if - - select type(cb => system%cb) - class is (symba_cb) - select type(pl => system%pl) - class is (symba_pl) - select type(tp => system%tp) - class is (symba_tp) - do - lmatch = .false. - read(LUN, iostat=ierr) id - if (ierr /=0) exit - - if (idx == cb%id) then - read(LUN) cb%info - lmatch = .true. - else - if (pl%nbody > 0) then - idx = findloc(pl%id(:), id, dim=1) - if (idx /= 0) then - read(LUN) pl%info(idx) - lmatch = .true. - end if - end if - if (.not.lmatch .and. tp%nbody > 0) then - idx = findloc(tp%id(:), id, dim=1) - if (idx /= 0) then - read(LUN) tp%info(idx) - lmatch = .true. - end if - end if - end if - if (.not.lmatch) then - write(*,*) 'Particle id ',id,' not found. Skipping' - read(LUN) tmpinfo - end if - end do - close(unit = LUN, iostat = ierr) - end select - end select - end select - if (ierr /= 0) then - write(*, *) "Swiftest error:" - write(*, *) " unable to close particle output file" - call util_exit(FAILURE) - end if - - return - end subroutine symba_io_read_particle - - module subroutine symba_io_write_discard(self, param) implicit none class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals integer(I4B), parameter :: LUN = 40 - integer(I4B) :: iadd, isub, j, ierr, nsub, nadd + integer(I4B) :: iadd, isub, j, nsub, nadd logical, save :: lfirst = .true. real(DP), dimension(:,:), allocatable :: vh character(*), parameter :: HDRFMT = '(E23.16, 1X, I8, 1X, L1)' @@ -343,17 +197,33 @@ module subroutine symba_io_write_discard(self, param) character(*), parameter :: NPLFMT = '(I8)' character(*), parameter :: PLNAMEFMT = '(I8, 2(1X, E23.16))' class(swiftest_body), allocatable :: pltemp + character(STRMAX) :: errmsg, out_stat associate(pl => self%pl, npl => self%pl%nbody, pl_adds => self%pl_adds) + if (self%tp_discards%nbody > 0) call io_write_discard(self, param) select type(pl_discards => self%pl_discards) class is (symba_merger) if (pl_discards%nbody == 0) return - select case(param%out_stat) + + ! Record the discarded body metadata information to file + if ((param%out_type == NETCDF_FLOAT_TYPE) .or. (param%out_type == NETCDF_DOUBLE_TYPE)) then + call param%nciu%open(param) + call pl_discards%write_particle_info(param%nciu) + call param%nciu%close(param) + end if + + if (param%discard_out == "") return + if (lfirst) then + out_stat = param%out_stat + else + out_stat = 'APPEND' + end if + select case(out_stat) case('APPEND') - open(unit = LUN, file = param%discard_out, status = 'OLD', position = 'APPEND', form = 'FORMATTED', iostat = ierr) + open(unit = LUN, file = param%discard_out, status = 'OLD', position = 'APPEND', form = 'FORMATTED', err = 667, iomsg = errmsg) case('NEW', 'REPLACE', 'UNKNOWN') - open(unit = LUN, file = param%discard_out, status = param%out_stat, form = 'FORMATTED', iostat = ierr) + open(unit = LUN, file = param%discard_out, status = param%out_stat, form = 'FORMATTED', err = 667, iomsg = errmsg) case default write(*,*) 'Invalid status code for OUT_STAT: ',trim(adjustl(param%out_stat)) call util_exit(FAILURE) @@ -364,7 +234,7 @@ module subroutine symba_io_write_discard(self, param) call pl_adds%pv2v(param) end if - write(LUN, HDRFMT) param%t, pl_discards%nbody, param%lbig_discard + write(LUN, HDRFMT, err = 667, iomsg = errmsg) param%t, pl_discards%nbody, param%lbig_discard iadd = 1 isub = 1 do while (iadd <= pl_adds%nbody) @@ -372,9 +242,9 @@ module subroutine symba_io_write_discard(self, param) nsub = pl_discards%ncomp(isub) do j = 1, nadd if (iadd <= pl_adds%nbody) then - write(LUN, NAMEFMT) ADD, pl_adds%id(iadd), pl_adds%status(iadd) - write(LUN, VECFMT) pl_adds%xh(1, iadd), pl_adds%xh(2, iadd), pl_adds%xh(3, iadd) - write(LUN, VECFMT) pl_adds%vh(1, iadd), pl_adds%vh(2, iadd), pl_adds%vh(3, iadd) + write(LUN, NAMEFMT, err = 667, iomsg = errmsg) ADD, pl_adds%id(iadd), pl_adds%status(iadd) + write(LUN, VECFMT, err = 667, iomsg = errmsg) pl_adds%xh(1, iadd), pl_adds%xh(2, iadd), pl_adds%xh(3, iadd) + write(LUN, VECFMT, err = 667, iomsg = errmsg) pl_adds%vh(1, iadd), pl_adds%vh(2, iadd), pl_adds%vh(3, iadd) else exit end if @@ -382,9 +252,9 @@ module subroutine symba_io_write_discard(self, param) end do do j = 1, nsub if (isub <= pl_discards%nbody) then - write(LUN, NAMEFMT) SUB, pl_discards%id(isub), pl_discards%status(isub) - write(LUN, VECFMT) pl_discards%xh(1, isub), pl_discards%xh(2, isub), pl_discards%xh(3, isub) - write(LUN, VECFMT) pl_discards%vh(1, isub), pl_discards%vh(2, isub), pl_discards%vh(3, isub) + write(LUN, NAMEFMT, err = 667, iomsg = errmsg) SUB, pl_discards%id(isub), pl_discards%status(isub) + write(LUN, VECFMT, err = 667, iomsg = errmsg) pl_discards%xh(1, isub), pl_discards%xh(2, isub), pl_discards%xh(3, isub) + write(LUN, VECFMT, err = 667, iomsg = errmsg) pl_discards%vh(1, isub), pl_discards%vh(2, isub), pl_discards%vh(3, isub) else exit end if @@ -397,6 +267,10 @@ module subroutine symba_io_write_discard(self, param) end associate return + + 667 continue + write(*,*) "Error writing discard file: " // trim(adjustl(errmsg)) + call util_exit(FAILURE) end subroutine symba_io_write_discard end submodule s_symba_io diff --git a/src/symba/symba_kick.f90 b/src/symba/symba_kick.f90 index 8625b3d81..2c074cb0d 100644 --- a/src/symba/symba_kick.f90 +++ b/src/symba/symba_kick.f90 @@ -2,6 +2,23 @@ use swiftest contains + module subroutine symba_kick_getacch_int_pl(self) + !! author: David A. Minton + !! + !! Compute direct cross (third) term heliocentric accelerations of massive bodies, with no mutual interactions between bodies below GMTINY + !! + !! Adapted from Hal Levison's Swift routine symba5_helio_getacch.f + !! Adapted from David E. Kaufmann's Swifter routine helio_kick_getacch_int.f90 + implicit none + ! Arguments + class(symba_pl), intent(inout) :: self + + call kick_getacch_int_all_pl(self%nbody, self%nplplm, self%k_plpl, self%xh, self%Gmass, self%radius, self%ah) + + return + end subroutine symba_kick_getacch_int_pl + + module subroutine symba_kick_getacch_pl(self, system, param, t, lbeg) !! author: David A. Minton !! @@ -17,27 +34,27 @@ module subroutine symba_kick_getacch_pl(self, system, param, t, lbeg) real(DP), intent(in) :: t !! Current simulation time logical, intent(in) :: lbeg !! Logical flag that determines whether or not this is the beginning or end of the step ! Internals - integer(I4B) :: k - real(DP) :: irij3, rji2, rlim2, faci, facj - real(DP), dimension(NDIM) :: dx + integer(I4B) :: i, j + integer(I8B) :: k, nplplenc + real(DP) :: rjj, rlim2, xr, yr, zr + real(DP), dimension(NDIM,self%nbody) :: ah_enc + integer(I4B), dimension(:,:), allocatable :: k_plpl_enc if (self%nbody == 0) return select type(system) class is (symba_nbody_system) - associate(pl => self, cb => system%cb, plplenc_list => system%plplenc_list, nplplenc => system%plplenc_list%nenc) + associate(pl => self, npl => self%nbody, plplenc_list => system%plplenc_list, radius => self%radius) + ! Apply kicks to all bodies (including those in the encounter list) call helio_kick_getacch_pl(pl, system, param, t, lbeg) - ! Remove accelerations from encountering pairs - do k = 1, nplplenc - associate(i => plplenc_list%index1(k), j => plplenc_list%index2(k)) - dx(:) = pl%xh(:, j) - pl%xh(:, i) - rji2 = dot_product(dx(:), dx(:)) - irij3 = 1.0_DP / (rji2 * sqrt(rji2)) - faci = pl%Gmass(i) * irij3 - facj = pl%Gmass(j) * irij3 - pl%ah(:, i) = pl%ah(:, i) - facj * dx(:) - pl%ah(:, j) = pl%ah(:, j) + faci * dx(:) - end associate - end do + + ! Remove kicks from bodies involved currently in the encounter list, as these are dealt with separately. + nplplenc = int(plplenc_list%nenc, kind=I8B) + allocate(k_plpl_enc(2,nplplenc)) + k_plpl_enc(:,1:nplplenc) = pl%k_plpl(:,plplenc_list%kidx(1:nplplenc)) + ah_enc(:,:) = 0.0_DP + call kick_getacch_int_all_pl(npl, nplplenc, k_plpl_enc, pl%xh, pl%Gmass, pl%radius, ah_enc) + pl%ah(:,1:npl) = pl%ah(:,1:npl) - ah_enc(:,1:npl) + end associate end select @@ -60,8 +77,8 @@ module subroutine symba_kick_getacch_tp(self, system, param, t, lbeg) real(DP), intent(in) :: t !! Current time logical, intent(in) :: lbeg !! Logical flag that determines whether or not this is the beginning or end of the step ! Internals - integer(I4B) :: k - real(DP) :: rji2, fac, rlim2 + integer(I4B) :: i, j, k + real(DP) :: rjj, fac, rlim2 real(DP), dimension(NDIM) :: dx if (self%nbody == 0) return @@ -71,18 +88,18 @@ module subroutine symba_kick_getacch_tp(self, system, param, t, lbeg) call helio_kick_getacch_tp(tp, system, param, t, lbeg) ! Remove accelerations from encountering pairs do k = 1, npltpenc - associate(i => pltpenc_list%index1(k), j => pltpenc_list%index2(k)) - if (tp%lmask(j)) THEN - if (lbeg) then - dx(:) = tp%xh(:,j) - pl%xbeg(:,i) - else - dx(:) = tp%xh(:,j) - pl%xend(:,i) - end if - rji2 = dot_product(dx(:), dx(:)) - fac = pl%Gmass(i) / (rji2 * sqrt(rji2)) - tp%ah(:,j) = tp%ah(:,j) + fac * dx(:) - end IF - end associate + i = pltpenc_list%index1(k) + j = pltpenc_list%index2(k) + if (tp%lmask(j)) THEN + if (lbeg) then + dx(:) = tp%xh(:,j) - pl%xbeg(:,i) + else + dx(:) = tp%xh(:,j) - pl%xend(:,i) + end if + rjj = dot_product(dx(:), dx(:)) + fac = pl%Gmass(i) / (rjj * sqrt(rjj)) + tp%ah(:,j) = tp%ah(:,j) + fac * dx(:) + end IF end do end associate end select @@ -90,7 +107,7 @@ module subroutine symba_kick_getacch_tp(self, system, param, t, lbeg) end subroutine symba_kick_getacch_tp - module subroutine symba_kick_pltpenc(self, system, dt, irec, sgn) + module subroutine symba_kick_encounter(self, system, dt, irec, sgn) !! author: David A. Minton !! !! Kick barycentric velocities of massive bodies and ACTIVE test particles within SyMBA recursion. @@ -100,19 +117,23 @@ module subroutine symba_kick_pltpenc(self, system, dt, irec, sgn) !! Adapted from Hal Levison's Swift routine symba5_kick.f implicit none ! Arguments - class(symba_pltpenc), intent(in) :: self !! SyMBA pl-tp encounter list object + class(symba_encounter), intent(in) :: self !! SyMBA pl-tp encounter list object class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - real(DP), intent(in) :: dt !! step size - integer(I4B), intent(in) :: irec !! Current recursion level - integer(I4B), intent(in) :: sgn !! sign to be applied to acceleration + real(DP), intent(in) :: dt !! step size + integer(I4B), intent(in) :: irec !! Current recursion level + integer(I4B), intent(in) :: sgn !! sign to be applied to acceleration ! Internals - integer(I4B) :: k, irm1, irecl + integer(I4B) :: i, j, irm1, irecl, ngood + integer(I8B) :: k real(DP) :: r, rr, ri, ris, rim1, r2, ir3, fac, faci, facj real(DP), dimension(NDIM) :: dx - logical :: isplpl, lgoodlevel + logical :: isplpl + logical, dimension(:), allocatable :: lgoodlevel + integer(I4B), dimension(:), allocatable :: good_idx if (self%nenc == 0) return + select type(self) class is (symba_plplenc) isplpl = .true. @@ -123,42 +144,67 @@ module subroutine symba_kick_pltpenc(self, system, dt, irec, sgn) class is (symba_pl) select type(tp => system%tp) class is (symba_tp) - associate(ind1 => self%index1, ind2 => self%index2) - if (pl%nbody > 0) pl%lmask(:) = pl%status(:) /= INACTIVE - if (tp%nbody > 0) tp%lmask(:) = tp%status(:) /= INACTIVE + associate(npl => pl%nbody, ntp => tp%nbody, nenc => self%nenc) + if (npl > 0) pl%lmask(1:npl) = pl%status(1:npl) /= INACTIVE + if (ntp > 0) tp%lmask(1:ntp) = tp%status(1:ntp) /= INACTIVE + allocate(lgoodlevel(nenc)) irm1 = irec - 1 + if (sgn < 0) then irecl = irec - 1 else irecl = irec end if - do k = 1, self%nenc + + do k = 1, nenc + i = self%index1(k) + j = self%index2(k) if (isplpl) then - pl%ah(:,ind1(k)) = 0.0_DP - pl%ah(:,ind2(k)) = 0.0_DP + lgoodlevel(k) = (pl%levelg(i) >= irm1) .and. (pl%levelg(j) >= irm1) else - tp%ah(:,ind2(k)) = 0.0_DP + lgoodlevel(k) = (pl%levelg(i) >= irm1) .and. (tp%levelg(j) >= irm1) end if + lgoodlevel(k) = (self%status(k) == ACTIVE) .and. lgoodlevel(k) + end do + ngood = count(lgoodlevel(:)) + if (ngood > 0_I8B) then + allocate(good_idx(ngood)) + good_idx(:) = pack([(i, i = 1, nenc)], lgoodlevel(:)) + if (isplpl) then - lgoodlevel = (pl%levelg(ind1(k)) >= irm1) .and. (pl%levelg(ind2(k)) >= irm1) + do concurrent (k = 1:ngood) + i = self%index1(good_idx(k)) + j = self%index2(good_idx(k)) + pl%ah(:,i) = 0.0_DP + pl%ah(:,j) = 0.0_DP + end do else - lgoodlevel = (pl%levelg(ind1(k)) >= irm1) .and. (tp%levelg(ind2(k)) >= irm1) + do concurrent (k = 1_I8B:ngood) + j = self%index2(good_idx(k)) + tp%ah(:,j) = 0.0_DP + end do end if - if ((self%status(k) /= INACTIVE) .and. lgoodlevel) then + + do k = 1, ngood + i = self%index1(good_idx(k)) + j = self%index2(good_idx(k)) if (isplpl) then - ri = ((pl%rhill(ind1(k)) + pl%rhill(ind2(k)))**2) * (RHSCALE**2) * (RSHELL**(2*irecl)) + ri = ((pl%rhill(i) + pl%rhill(j))**2) * (RHSCALE**2) * (RSHELL**(2*irecl)) rim1 = ri * (RSHELL**2) - dx(:) = pl%xh(:,ind2(k)) - pl%xh(:,ind1(k)) + dx(:) = pl%xh(:,j) - pl%xh(:,i) else - ri = ((pl%rhill(ind1(k)))**2) * (RHSCALE**2) * (RSHELL**(2*irecl)) + ri = ((pl%rhill(i))**2) * (RHSCALE**2) * (RSHELL**(2*irecl)) rim1 = ri * (RSHELL**2) - dx(:) = tp%xh(:,ind2(k)) - pl%xh(:,ind1(k)) + dx(:) = tp%xh(:,j) - pl%xh(:,i) end if r2 = dot_product(dx(:), dx(:)) if (r2 < rim1) then fac = 0.0_DP - else if (r2 < ri) then + lgoodlevel(good_idx(k)) = .false. + cycle + end if + if (r2 < ri) then ris = sqrt(ri) r = sqrt(r2) rr = (ris - r) / (ris * (1.0_DP - RSHELL)) @@ -167,34 +213,41 @@ module subroutine symba_kick_pltpenc(self, system, dt, irec, sgn) ir3 = 1.0_DP / (r2 * sqrt(r2)) fac = ir3 end if - faci = fac * pl%Gmass(ind1(k)) + faci = fac * pl%Gmass(i) if (isplpl) then - facj = fac * pl%Gmass(ind2(k)) - pl%ah(:,ind1(k)) = pl%ah(:,ind1(k)) + facj * dx(:) - pl%ah(:,ind2(k)) = pl%ah(:,ind2(k)) - faci * dx(:) + facj = fac * pl%Gmass(j) + pl%ah(:, i) = pl%ah(:, i) + facj * dx(:) + pl%ah(:, j) = pl%ah(:, j) - faci * dx(:) else - tp%ah(:,ind2(k)) = tp%ah(:,ind2(k)) - faci * dx(:) + tp%ah(:, j) = tp%ah(:, j) - faci * dx(:) end if - end if - end do - if (isplpl) then - do k = 1, self%nenc - pl%vb(:,ind1(k)) = pl%vb(:,ind1(k)) + sgn * dt * pl%ah(:,ind1(k)) - pl%vb(:,ind2(k)) = pl%vb(:,ind2(k)) + sgn * dt * pl%ah(:,ind2(k)) - pl%ah(:,ind1(k)) = 0.0_DP - pl%ah(:,ind1(k)) = 0.0_DP - end do - else - do k = 1, self%nenc - tp%vb(:,ind2(k)) = tp%vb(:,ind2(k)) + sgn * dt * tp%ah(:,ind2(k)) - tp%ah(:,ind2(k)) = 0.0_DP end do + ngood = count(lgoodlevel(:)) + if (ngood == 0_I8B) return + good_idx(1:ngood) = pack([(i, i = 1, nenc)], lgoodlevel(:)) + + if (isplpl) then + do k = 1, ngood + i = self%index1(good_idx(k)) + j = self%index2(good_idx(k)) + pl%vb(:,i) = pl%vb(:,i) + sgn * dt * pl%ah(:,i) + pl%vb(:,j) = pl%vb(:,j) + sgn * dt * pl%ah(:,j) + pl%ah(:,i) = 0.0_DP + pl%ah(:,j) = 0.0_DP + end do + else + do k = 1, ngood + j = self%index2(good_idx(k)) + tp%vb(:,j) = tp%vb(:,j) + sgn * dt * tp%ah(:,j) + tp%ah(:,j) = 0.0_DP + end do + end if end if end associate end select end select return - end subroutine symba_kick_pltpenc + end subroutine symba_kick_encounter end submodule s_symba_kick \ No newline at end of file diff --git a/src/symba/symba_setup.f90 b/src/symba/symba_setup.f90 index e06fb20b5..3a0543ee1 100644 --- a/src/symba/symba_setup.f90 +++ b/src/symba/symba_setup.f90 @@ -2,62 +2,6 @@ use swiftest contains - module subroutine symba_setup_initialize_particle_info(system, param) - !! author: David A. Minton - !! - !! Initializes a new particle information data structure with initial conditions recorded - implicit none - ! Argumets - class(symba_nbody_system), intent(inout) :: system !! SyMBA nbody system object - class(symba_parameters), intent(inout) :: param !! Current run configuration parameters with SyMBA extensions - ! Internals - integer(I4B) :: i - integer(I4B), dimension(:), allocatable :: idx - - select type(cb => system%cb) - class is (symba_cb) - cb%info%origin_type = "Central body" - cb%info%origin_time = param%t0 - cb%info%origin_xh(:) = 0.0_DP - cb%info%origin_vh(:) = 0.0_DP - call symba_io_dump_particle_info(system, param, lincludecb=.true.) - end select - - select type(pl => system%pl) - class is (symba_pl) - do i = 1, pl%nbody - pl%info(i)%origin_type = "Initial conditions" - pl%info(i)%origin_time = param%t0 - pl%info(i)%origin_xh(:) = pl%xh(:,i) - pl%info(i)%origin_vh(:) = pl%vh(:,i) - end do - if (pl%nbody > 0) then - allocate(idx(pl%nbody)) - call symba_io_dump_particle_info(system, param, plidx=[(i, i=1, pl%nbody)]) - deallocate(idx) - end if - end select - - select type(tp => system%tp) - class is (symba_tp) - do i = 1, tp%nbody - tp%info(i)%origin_type = "Initial conditions" - tp%info(i)%origin_time = param%t0 - tp%info(i)%origin_xh(:) = tp%xh(:,i) - tp%info(i)%origin_vh(:) = tp%vh(:,i) - end do - if (tp%nbody > 0) then - allocate(idx(tp%nbody)) - call symba_io_dump_particle_info(system, param, tpidx=[(i, i=1, tp%nbody)]) - deallocate(idx) - end if - end select - - - return - end subroutine symba_setup_initialize_particle_info - - module subroutine symba_setup_initialize_system(self, param) !! author: David A. Minton !! @@ -73,23 +17,10 @@ module subroutine symba_setup_initialize_system(self, param) ! Call parent method associate(system => self) - call whm_setup_initialize_system(system, param) + call helio_setup_initialize_system(system, param) call system%pltpenc_list%setup(0) call system%plplenc_list%setup(0) - select type(pl => system%pl) - class is (symba_pl) - call pl%sort("mass", ascending=.false.) - select type(param) - class is (symba_parameters) - pl%lmtiny(:) = pl%Gmass(:) > param%GMTINY - pl%nplm = count(pl%lmtiny(:)) - if (param%lrestart) then - call symba_io_read_particle(system, param) - else - call symba_setup_initialize_particle_info(system, param) - end if - end select - end select + call system%plplcollision_list%setup(0) end associate return @@ -112,9 +43,12 @@ module subroutine symba_setup_merger(self, n, param) !> Call allocation method for parent class. In this case, helio_pl does not have its own setup method so we use the base method for swiftest_pl call symba_setup_pl(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%ncomp)) deallocate(self%ncomp) + + if (n == 0) return + allocate(self%ncomp(n)) self%ncomp(:) = 0 @@ -138,7 +72,7 @@ module subroutine symba_setup_pl(self, n, param) !> Call allocation method for parent class. In this case, helio_pl does not have its own setup method so we use the base method for swiftest_pl call setup_pl(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%lcollision)) deallocate(self%lcollision) if (allocated(self%lencounter)) deallocate(self%lencounter) @@ -151,7 +85,8 @@ module subroutine symba_setup_pl(self, n, param) if (allocated(self%peri)) deallocate(self%peri) if (allocated(self%atp)) deallocate(self%atp) if (allocated(self%kin)) deallocate(self%kin) - if (allocated(self%info)) deallocate(self%info) + + if (n == 0) return allocate(self%lcollision(n)) allocate(self%lencounter(n)) @@ -164,7 +99,6 @@ module subroutine symba_setup_pl(self, n, param) allocate(self%peri(n)) allocate(self%atp(n)) allocate(self%kin(n)) - allocate(self%info(n)) self%lcollision(:) = .false. self%lencounter(:) = .false. @@ -176,32 +110,34 @@ module subroutine symba_setup_pl(self, n, param) self%isperi(:) = 0 self%peri(:) = 0.0_DP self%atp(:) = 0.0_DP - self%kin(:)%nchild = 0 - self%kin(:)%parent = [(i, i=1, n)] + call self%reset_kinship([(i, i=1, n)]) return end subroutine symba_setup_pl - module subroutine symba_setup_pltpenc(self, n) + module subroutine symba_setup_encounter(self, n) !! author: David A. Minton !! !! A constructor that sets the number of encounters and allocates and initializes all arrays !! implicit none ! Arguments - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter structure + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter structure integer(I4B), intent(in) :: n !! Number of encounters to allocate space for call setup_encounter(self, n) - if (n == 0) return + if (n < 0) return if (allocated(self%level)) deallocate(self%level) + + if (n ==0) return + allocate(self%level(n)) self%level(:) = -1 return - end subroutine symba_setup_pltpenc + end subroutine symba_setup_encounter module subroutine symba_setup_tp(self, n, param) @@ -218,13 +154,15 @@ module subroutine symba_setup_tp(self, n, param) !> Call allocation method for parent class. In this case, helio_tp does not have its own setup method so we use the base method for swiftest_tp call setup_tp(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%nplenc)) deallocate(self%nplenc) if (allocated(self%levelg)) deallocate(self%levelg) if (allocated(self%levelm)) deallocate(self%levelm) if (allocated(self%info)) deallocate(self%info) + if (n == 0) return + allocate(self%nplenc(n)) allocate(self%levelg(n)) allocate(self%levelm(n)) diff --git a/src/symba/symba_step.f90 b/src/symba/symba_step.f90 index 7065625b4..9f4508550 100644 --- a/src/symba/symba_step.f90 +++ b/src/symba/symba_step.f90 @@ -19,20 +19,22 @@ module subroutine symba_step_system(self, param, t, dt) ! Internals logical :: lencounter - call self%reset() select type(pl => self%pl) class is (symba_pl) select type(tp => self%tp) class is (symba_tp) - lencounter = pl%encounter_check(self, dt, 0) .or. tp%encounter_check(self, dt, 0) - if (lencounter) then - tp%lfirst = pl%lfirst - call self%interp(param, t, dt) - pl%lfirst = .true. - tp%lfirst = .true. - else - call helio_step_system(self, param, t, dt) - end if + select type(param) + class is (symba_parameters) + call self%reset(param) + lencounter = pl%encounter_check(self, dt, 0) .or. tp%encounter_check(self, dt, 0) + if (lencounter) then + call self%interp(param, t, dt) + param%lfirstkick = .true. + else + self%irec = -1 + call helio_step_system(self, param, t, dt) + end if + end select end select end select @@ -108,32 +110,17 @@ module subroutine symba_step_set_recur_levels_system(self, ireci) ! Internals integer(I4B) :: k, irecp - associate(system => self, plplenc_list => self%plplenc_list, pltpenc_list => self%pltpenc_list) + associate(system => self, plplenc_list => self%plplenc_list, pltpenc_list => self%pltpenc_list, npl => self%pl%nbody, ntp => self%tp%nbody) select type(pl => self%pl) class is (symba_pl) select type(tp => self%tp) class is (symba_tp) irecp = ireci + 1 - if (plplenc_list%nenc > 0) then - do k = 1, plplenc_list%nenc - associate(i => plplenc_list%index1(k), j => plplenc_list%index2(k)) - if (pl%levelg(i) == irecp) pl%levelg(i) = ireci - if (pl%levelg(j) == irecp) pl%levelg(j) = ireci - end associate - end do - where(plplenc_list%level(1:plplenc_list%nenc) == irecp) plplenc_list%level(1:plplenc_list%nenc) = ireci - end if - - if (pltpenc_list%nenc > 0) then - do k = 1, pltpenc_list%nenc - associate(i => pltpenc_list%index1(k), j => pltpenc_list%index2(k)) - if (pl%levelg(i) == irecp) pl%levelg(i) = ireci - if (tp%levelg(j) == irecp) tp%levelg(j) = ireci - end associate - end do - where(pltpenc_list%level(1:pltpenc_list%nenc) == irecp) pltpenc_list%level(1:pltpenc_list%nenc) = ireci - end if + if (npl >0) where(pl%levelg(1:npl) == irecp) pl%levelg(1:npl) = ireci + if (ntp > 0) where(tp%levelg(1:ntp) == irecp) tp%levelg(1:ntp) = ireci + if (plplenc_list%nenc > 0) where(plplenc_list%level(1:plplenc_list%nenc) == irecp) plplenc_list%level(1:plplenc_list%nenc) = ireci + if (pltpenc_list%nenc > 0) where(pltpenc_list%level(1:pltpenc_list%nenc) == irecp) pltpenc_list%level(1:pltpenc_list%nenc) = ireci system%irec = ireci @@ -157,13 +144,13 @@ module recursive subroutine symba_step_recur_system(self, param, t, ireci) ! Arguments class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters - real(DP), value :: t - integer(I4B), value :: ireci !! input recursion level + real(DP), intent(in) :: t + integer(I4B), intent(in) :: ireci !! input recursion level ! Internals integer(I4B) :: i, j, irecp, nloops real(DP) :: dtl, dth real(DP), dimension(NDIM) :: xr, vr - logical :: lencounter + logical :: lencounter, lplpl_collision, lpltp_collision associate(system => self, plplenc_list => self%plplenc_list, pltpenc_list => self%pltpenc_list) select type(pl => self%pl) @@ -209,8 +196,11 @@ module recursive subroutine symba_step_recur_system(self, param, t, ireci) end if if (param%lclose) then - call plplenc_list%collision_check(system, param, t+dtl, dtl, ireci) - call pltpenc_list%collision_check(system, param, t+dtl, dtl, ireci) + lplpl_collision = plplenc_list%collision_check(system, param, t+dtl, dtl, ireci) + lpltp_collision = pltpenc_list%collision_check(system, param, t+dtl, dtl, ireci) + + if (lplpl_collision) call plplenc_list%resolve_collision(system, param, t+dtl, dtl, ireci) + if (lpltp_collision) call pltpenc_list%resolve_collision(system, param, t+dtl, dtl, ireci) end if call self%set_recur_levels(ireci) @@ -224,7 +214,7 @@ module recursive subroutine symba_step_recur_system(self, param, t, ireci) end subroutine symba_step_recur_system - module subroutine symba_step_reset_system(self) + module subroutine symba_step_reset_system(self, param) !! author: David A. Minton !! !! Resets pl, tp,and encounter structures at the start of a new step @@ -233,40 +223,53 @@ module subroutine symba_step_reset_system(self) !! Adapted from Hal Levison's Swift routine symba5_step.f implicit none ! Arguments - class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object + class(symba_nbody_system), intent(inout) :: self !! SyMBA nbody system object + class(symba_parameters), intent(in) :: param !! Current run configuration parameters with SyMBA additions ! Internals - integer(I4B) :: i + integer(I4B) :: i, nenc_old - associate(system => self, pltpenc_list => self%pltpenc_list, plplenc_list => self%plplenc_list, pl_adds => self%pl_adds, pl_discards => self%pl_discards) + associate(system => self) select type(pl => system%pl) class is (symba_pl) select type(tp => system%tp) class is (symba_tp) - if (pl%nbody > 0) then - pl%lcollision(:) = .false. - pl%kin(:)%parent = [(i, i=1, pl%nbody)] - pl%kin(:)%nchild = 0 - do i = 1, pl%nbody - if (allocated(pl%kin(i)%child)) deallocate(pl%kin(i)%child) - end do - pl%nplenc(:) = 0 - pl%ntpenc(:) = 0 - pl%levelg(:) = 0 - pl%levelm(:) = 0 - pl%lencounter = .false. - pl%lcollision = .false. - plplenc_list%nenc = 0 - end if - - if (tp%nbody > 0) then - tp%nplenc(:) = 0 - tp%levelg(:) = 0 - tp%levelm(:) = 0 - pltpenc_list%nenc = 0 - end if + associate(npl => pl%nbody, ntp => tp%nbody) + if (npl > 0) then + pl%lcollision(1:npl) = .false. + call pl%reset_kinship([(i, i=1, npl)]) + pl%nplenc(1:npl) = 0 + pl%ntpenc(1:npl) = 0 + pl%levelg(1:npl) = -1 + pl%levelm(1:npl) = -1 + pl%lencounter(1:npl) = .false. + pl%lcollision(1:npl) = .false. + pl%ldiscard(1:npl) = .false. + pl%lmask(1:npl) = .true. + nenc_old = system%plplenc_list%nenc + call system%plplenc_list%setup(0) + call system%plplenc_list%setup(nenc_old) + system%plplenc_list%nenc = 0 + call system%plplcollision_list%setup(0) + end if + + if (ntp > 0) then + tp%nplenc(1:ntp) = 0 + tp%levelg(1:ntp) = -1 + tp%levelm(1:ntp) = -1 + tp%lmask(1:ntp) = .true. + tp%ldiscard(1:npl) = .false. + nenc_old = system%pltpenc_list%nenc + call system%pltpenc_list%setup(0) + call system%pltpenc_list%setup(nenc_old) + system%pltpenc_list%nenc = 0 + end if + + call system%pl_adds%setup(0, param) + call system%pl_discards%setup(0, param) - call pl_adds%resize(0) - call pl_discards%resize(0) + tp%lfirst = param%lfirstkick + pl%lfirst = param%lfirstkick + end associate end select end select end associate diff --git a/src/symba/symba_util.f90 b/src/symba/symba_util.f90 index 4c0f256e3..8b8e48f47 100644 --- a/src/symba/symba_util.f90 +++ b/src/symba/symba_util.f90 @@ -2,30 +2,6 @@ use swiftest contains - module subroutine symba_util_append_arr_info(arr, source, nold, nsrc, lsource_mask) - !! author: David A. Minton - !! - !! Append a single array of particle information type onto another. If the destination array is not allocated, or is not big enough, this will allocate space for it. - implicit none - ! Arguments - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array - type(symba_particle_info), dimension(:), allocatable, intent(in) :: source !! Array to append - integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively - logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to - - if (.not. allocated(source)) return - - if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) - else - call util_resize(arr, nold + nsrc) - end if - - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) - - return - end subroutine symba_util_append_arr_info - module subroutine symba_util_append_arr_kin(arr, source, nold, nsrc, lsource_mask) !! author: David A. Minton @@ -37,21 +13,47 @@ module subroutine symba_util_append_arr_kin(arr, source, nold, nsrc, lsource_mas type(symba_kinship), dimension(:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) + allocate(arr(nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) + arr(nold + 1:nold + nnew) = pack(source(1:nsrc), lsource_mask(1:nsrc)) return end subroutine symba_util_append_arr_kin + module subroutine symba_util_append_encounter(self, source, lsource_mask) + !! author: David A. Minton + !! + !! Append components from one encounter list (pl-pl or pl-tp) body object to another. + !! This method will automatically resize the destination body if it is too small + implicit none + ! Arguments + class(symba_encounter), intent(inout) :: self !! SyMBA encounter list object + class(swiftest_encounter), intent(in) :: source !! Source object to append + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + + associate(nold => self%nenc, nsrc => source%nenc) + select type(source) + class is (symba_encounter) + call util_append(self%level, source%level, nold, nsrc, lsource_mask) + end select + call util_append_encounter(self, source, lsource_mask) + end associate + + return + end subroutine symba_util_append_encounter + + module subroutine symba_util_append_pl(self, source, lsource_mask) !! author: David A. Minton !! @@ -77,7 +79,6 @@ module subroutine symba_util_append_pl(self, source, lsource_mask) call util_append(self%peri, source%peri, nold, nsrc, lsource_mask) call util_append(self%atp, source%atp, nold, nsrc, lsource_mask) call util_append(self%kin, source%kin, nold, nsrc, lsource_mask) - call util_append(self%info, source%info, nold, nsrc, lsource_mask) call util_append_pl(self, source, lsource_mask) ! Note: helio_pl does not have its own append method, so we skip back to the base class end associate @@ -102,10 +103,12 @@ module subroutine symba_util_append_merger(self, source, lsource_mask) logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to ! Internals integer(I4B), dimension(:), allocatable :: ncomp_tmp !! Temporary placeholder for ncomp incase we are appending a symba_pl object to a symba_merger - integer(I4B) :: nold, nsrc + integer(I4B) :: nold, nsrc, nnew nold = self%nbody nsrc = source%nbody + nnew = count(lsource_mask) + select type(source) class is (symba_merger) call util_append(self%ncomp, source%ncomp, nold, nsrc, lsource_mask) @@ -121,7 +124,7 @@ module subroutine symba_util_append_merger(self, source, lsource_mask) end select ! Save the number of appended bodies - self%ncomp(nold+1:nold+nsrc) = nsrc + self%ncomp(nold+1:nold+nnew) = nnew return end subroutine symba_util_append_merger @@ -144,7 +147,6 @@ module subroutine symba_util_append_tp(self, source, lsource_mask) call util_append(self%nplenc, source%nplenc, nold, nsrc, lsource_mask) call util_append(self%levelg, source%levelg, nold, nsrc, lsource_mask) call util_append(self%levelm, source%levelm, nold, nsrc, lsource_mask) - call util_append(self%info, source%info, nold, nsrc, lsource_mask) call util_append_tp(self, source, lsource_mask) ! Note: helio_tp does not have its own append method, so we skip back to the base class end associate @@ -157,24 +159,26 @@ module subroutine symba_util_append_tp(self, source, lsource_mask) end subroutine symba_util_append_tp - module subroutine symba_util_fill_arr_info(keeps, inserts, lfill_list) + module subroutine symba_util_copy_encounter(self, source) !! author: David A. Minton !! - !! Performs a fill operation on a single array of particle origin information types - !! This is the inverse of a spill operation + !! Copies elements from the source encounter list into self. implicit none ! Arguments - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep - type(symba_particle_info), dimension(:), allocatable, intent(in) :: inserts !! Array of values to insert into keep - logical, dimension(:), intent(in) :: lfill_list !! Logical array of bodies to merge into the keeps - - if (.not.allocated(keeps) .or. .not.allocated(inserts)) return + class(symba_encounter), intent(inout) :: self !! Encounter list + class(swiftest_encounter), intent(in) :: source !! Source object to copy into + + select type(source) + class is (symba_encounter) + associate(n => source%nenc) + self%level(1:n) = source%level(1:n) + end associate + end select - keeps(:) = unpack(keeps(:), .not.lfill_list(:), keeps(:)) - keeps(:) = unpack(inserts(:), lfill_list(:), keeps(:)) + call util_copy_encounter(self, source) return - end subroutine symba_util_fill_arr_info + end subroutine symba_util_copy_encounter module subroutine symba_util_fill_arr_kin(keeps, inserts, lfill_list) @@ -223,7 +227,6 @@ module subroutine symba_util_fill_pl(self, inserts, lfill_list) call util_fill(keeps%peri, inserts%peri, lfill_list) call util_fill(keeps%atp, inserts%atp, lfill_list) call util_fill(keeps%kin, inserts%kin, lfill_list) - call util_fill(keeps%info, inserts%info, lfill_list) call util_fill_pl(keeps, inserts, lfill_list) ! Note: helio_pl does not have its own fill method, so we skip back to the base class class default @@ -254,7 +257,6 @@ module subroutine symba_util_fill_tp(self, inserts, lfill_list) call util_fill(keeps%nplenc, inserts%nplenc, lfill_list) call util_fill(keeps%levelg, inserts%levelg, lfill_list) call util_fill(keeps%levelm, inserts%levelm, lfill_list) - call util_fill(keeps%info, inserts%info, lfill_list) call util_fill_tp(keeps, inserts, lfill_list) ! Note: helio_tp does not have its own fill method, so we skip back to the base class class default @@ -267,6 +269,47 @@ module subroutine symba_util_fill_tp(self, inserts, lfill_list) end subroutine symba_util_fill_tp + module subroutine symba_util_index_eucl_plpl(self, param) + !! author: Jacob R. Elliott and David A. Minton + !! + !! Turns i,j indices into k index for use in the Euclidean distance matrix. This also sets the lmtiny flag and computes the + !! number of interactions that excludes semi-interacting bodies with each other (Gmass < GMTINY). + !! This method will also sort the bodies in descending order by Mass + !! + !! Reference: + !! + !! Mélodie Angeletti, Jean-Marie Bonny, Jonas Koko. Parallel Euclidean distance matrix computation on big datasets *. + !! 2019. hal-0204751 + implicit none + ! Arguments + class(symba_pl), intent(inout) :: self !! SyMBA massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I8B) :: i, j, counter, npl, nplm, nplpl, nplplm + + associate(pl => self) + npl = int(self%nbody, kind=I8B) + nplm = count(.not. pl%lmtiny(1:npl)) + pl%nplm = int(nplm, kind=I4B) + + pl%nplpl = (npl * (npl - 1) / 2) ! number of entries in a strict lower triangle, npl x npl, minus first column + pl%nplplm = nplm * npl - nplm * (nplm + 1) / 2 ! number of entries in a strict lower triangle, npl x npl, minus first column including only mutually interacting bodies + if (allocated(self%k_plpl)) deallocate(self%k_plpl) ! Reset the index array if it's been set previously + allocate(self%k_plpl(2, pl%nplpl)) + do i = 1, npl + counter = (i - 1_I8B) * npl - i * (i - 1_I8B) / 2_I8B + 1_I8B + do j = i + 1_I8B, npl + self%k_plpl(1, counter) = i + self%k_plpl(2, counter) = j + counter = counter + 1_I8B + end do + end do + end associate + + return + end subroutine symba_util_index_eucl_plpl + + module subroutine symba_util_peri_pl(self, system, param) !! author: David A. Minton !! @@ -361,78 +404,165 @@ module subroutine symba_util_rearray_pl(self, system, param) ! Arguments class(symba_pl), intent(inout) :: self !! SyMBA massive body object class(symba_nbody_system), intent(inout) :: system !! Swiftest nbody system object - class(symba_parameters), intent(in) :: param !! Current run configuration parameters + class(symba_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals class(symba_pl), allocatable :: tmp !! The discarded body list. - integer(I4B) :: i - logical, dimension(:), allocatable :: lmask + integer(I4B) :: i, j, k, npl, nadd, nencmin, nenc_old, idnew1, idnew2, idold1, idold2 + logical, dimension(:), allocatable :: lmask, ldump_mask + class(symba_plplenc), allocatable :: plplenc_old + logical :: lencounter + integer(I4B), dimension(:), allocatable :: levelg_orig_pl, levelm_orig_pl, levelg_orig_tp, levelm_orig_tp, nplenc_orig_pl, nplenc_orig_tp, ntpenc_orig_pl associate(pl => self, pl_adds => system%pl_adds) - allocate(tmp, mold=pl) + + npl = pl%nbody + nadd = pl_adds%nbody + if (npl == 0) return + ! Deallocate any temporary variables + if (allocated(pl%xbeg)) deallocate(pl%xbeg) + if (allocated(pl%xend)) deallocate(pl%xend) + ! Remove the discards and destroy the list, as the system already tracks pl_discards elsewhere - allocate(lmask, source=pl%ldiscard(:)) - lmask(:) = lmask(:) .or. pl%status(:) == INACTIVE + allocate(lmask(npl)) + lmask(1:npl) = pl%ldiscard(1:npl) + allocate(tmp, mold=self) call pl%spill(tmp, lspill_list=lmask, ldestructive=.true.) + npl = pl%nbody call tmp%setup(0,param) deallocate(tmp) + deallocate(lmask) - ! Deallocate any temporary variables - if (allocated(pl%xbeg)) deallocate(pl%xbeg) - if (allocated(pl%xend)) deallocate(pl%xend) + ! Store the original plplenc list so we don't remove any of the original encounters + nenc_old = system%plplenc_list%nenc + if (nenc_old > 0) then + allocate(plplenc_old, source=system%plplenc_list) + call plplenc_old%copy(system%plplenc_list) + end if ! Add in any new bodies - if (pl_adds%nbody > 0) then - call pl%append(pl_adds, lsource_mask=[(.true., i=1, pl_adds%nbody)]) - call symba_io_dump_particle_info(system, param, plidx=[(i, i = 1, pl%nbody)]) - end if - - ! If there are still bodies in the system, sort by mass in descending order and re-index - if (pl%nbody > 0) then - call pl%sort("mass", ascending=.false.) - pl%lmtiny(:) = pl%Gmass(:) > param%GMTINY - pl%nplm = count(pl%lmtiny(:)) - call pl%eucl_index() + if (nadd > 0) then + ! Append the adds to the main pl object + call pl%append(pl_adds, lsource_mask=[(.true., i=1, nadd)]) + + allocate(ldump_mask(npl+nadd)) ! This mask is used only to append the original Fortran binary particle.dat file with new bodies. This is ignored for NetCDF output + ldump_mask(1:npl) = .false. + ldump_mask(npl+1:npl+nadd) = pl%status(npl+1:npl+nadd) == NEW_PARTICLE + npl = pl%nbody + else + allocate(ldump_mask(npl)) + ldump_mask(:) = .false. end if + ! Reset all of the status flags for this body + pl%status(1:npl) = ACTIVE + do i = 1, npl + call pl%info(i)%set_value(status="ACTIVE") + end do + pl%ldiscard(1:npl) = .false. + pl%lcollision(1:npl) = .false. + pl%lmask(1:npl) = .true. + + select type(param) + class is (symba_parameters) + pl%lmtiny(1:npl) = pl%Gmass(1:npl) < param%GMTINY + where(pl%lmtiny(1:npl)) + pl%info(1:npl)%particle_type = PL_TINY_TYPE_NAME + elsewhere + pl%info(1:npl)%particle_type = PL_TYPE_NAME + end where + end select + + call pl%dump_particle_info(param, idx=pack([(i, i=1, npl)], ldump_mask)) + deallocate(ldump_mask) + + ! Reindex the new list of bodies + call pl%sort("mass", ascending=.false.) + call pl%index(param) + + ! Reset the kinship trackers + call pl%reset_kinship([(i, i=1, npl)]) + + ! Re-build the zero-level encounter list, being sure to save the original level information for all bodies + allocate(levelg_orig_pl, source=pl%levelg) + allocate(levelm_orig_pl, source=pl%levelm) + allocate(nplenc_orig_pl, source=pl%nplenc) + lencounter = pl%encounter_check(system, param%dt, 0) + if (system%tp%nbody > 0) then + select type(tp => system%tp) + class is (symba_tp) + allocate(ntpenc_orig_pl, source=pl%ntpenc) + allocate(levelg_orig_tp, source=tp%levelg) + allocate(levelm_orig_tp, source=tp%levelm) + allocate(nplenc_orig_tp, source=tp%nplenc) + lencounter = tp%encounter_check(system, param%dt, 0) + call move_alloc(levelg_orig_tp, tp%levelg) + call move_alloc(levelm_orig_tp, tp%levelm) + call move_alloc(nplenc_orig_tp, tp%nplenc) + call move_alloc(ntpenc_orig_pl, pl%ntpenc) + end select + end if + call move_alloc(levelg_orig_pl, pl%levelg) + call move_alloc(levelm_orig_pl, pl%levelm) + call move_alloc(nplenc_orig_pl, pl%nplenc) + + ! Re-index the encounter list as the index values may have changed + if (nenc_old > 0) then + nencmin = min(system%plplenc_list%nenc, plplenc_old%nenc) + do k = 1, nencmin + idnew1 = system%plplenc_list%id1(k) + idnew2 = system%plplenc_list%id2(k) + idold1 = plplenc_old%id1(k) + idold2 = plplenc_old%id2(k) + if ((idnew1 == idold1) .and. (idnew2 == idold2)) then + ! This is an encounter we already know about, so save the old information + system%plplenc_list%lvdotr(k) = plplenc_old%lvdotr(k) + system%plplenc_list%status(k) = plplenc_old%status(k) + system%plplenc_list%x1(:,k) = plplenc_old%x1(:,k) + system%plplenc_list%x2(:,k) = plplenc_old%x2(:,k) + system%plplenc_list%v1(:,k) = plplenc_old%v1(:,k) + system%plplenc_list%v2(:,k) = plplenc_old%v2(:,k) + system%plplenc_list%t(k) = plplenc_old%t(k) + system%plplenc_list%level(k) = plplenc_old%level(k) + else if (((idnew1 == idold2) .and. (idnew2 == idold1))) then + ! This is an encounter we already know about, but with the order reversed, so save the old information + system%plplenc_list%lvdotr(k) = plplenc_old%lvdotr(k) + system%plplenc_list%status(k) = plplenc_old%status(k) + system%plplenc_list%x1(:,k) = plplenc_old%x2(:,k) + system%plplenc_list%x2(:,k) = plplenc_old%x1(:,k) + system%plplenc_list%v1(:,k) = plplenc_old%v2(:,k) + system%plplenc_list%v2(:,k) = plplenc_old%v1(:,k) + system%plplenc_list%t(k) = plplenc_old%t(k) + system%plplenc_list%level(k) = plplenc_old%level(k) + end if + end do + end if end associate return end subroutine symba_util_rearray_pl - module subroutine symba_util_resize_arr_info(arr, nnew) + module subroutine symba_util_reset_kinship(self, idx) !! author: David A. Minton + !! + !! Resets the kinship status of bodies. !! - !! Resizes an array component of type character string. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. implicit none - ! Arguments - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Array to resize - integer(I4B), intent(in) :: nnew !! New size + class(symba_pl), intent(inout) :: self !! SyMBA massive body object + integer(I4B), dimension(:), intent(in) :: idx !! Index array of bodies to reset ! Internals - type(symba_particle_info), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated - integer(I4B) :: nold !! Old size - - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr) - if (nnew == nold) return + integer(I4B) :: i, j - if (nnew == 0) then - deallocate(arr) - return - end if - - allocate(tmp(nnew)) - if (nnew > nold) then - tmp(1:nold) = arr(1:nold) - else - tmp(1:nnew) = arr(1:nnew) - end if - call move_alloc(tmp, arr) + self%kin(idx(:))%parent = idx(:) + self%kin(idx(:))%nchild = 0 + do j = 1, size(idx(:)) + i = idx(j) + if (allocated(self%kin(i)%child)) deallocate(self%kin(i)%child) + end do return - end subroutine symba_util_resize_arr_info - + end subroutine symba_util_reset_kinship + module subroutine symba_util_resize_arr_kin(arr, nnew) !! author: David A. Minton @@ -446,16 +576,19 @@ module subroutine symba_util_resize_arr_kin(arr, nnew) type(symba_kinship), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr) - if (nnew == nold) return + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if + allocate(tmp(nnew)) if (nnew > nold) then tmp(1:nold) = arr(1:nold) @@ -505,7 +638,6 @@ module subroutine symba_util_resize_pl(self, nnew) call util_resize(self%peri, nnew) call util_resize(self%atp, nnew) call util_resize(self%kin, nnew) - call util_resize(self%info, nnew) call util_resize_pl(self, nnew) @@ -525,7 +657,6 @@ module subroutine symba_util_resize_tp(self, nnew) call util_resize(self%nplenc, nnew) call util_resize(self%levelg, nnew) call util_resize(self%levelm, nnew) - call util_resize(self%info, nnew) call util_resize_tp(self, nnew) @@ -544,7 +675,7 @@ module subroutine symba_util_sort_pl(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction if (self%nbody == 0) return @@ -556,6 +687,7 @@ module subroutine symba_util_sort_pl(self, sortby, ascending) end if associate(pl => self, npl => self%nbody) + allocate(ind(npl)) select case(sortby) case("nplenc") call util_sort(direction * pl%nplenc(1:npl), ind(1:npl)) @@ -594,7 +726,7 @@ module subroutine symba_util_sort_tp(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction if (self%nbody == 0) return @@ -606,6 +738,7 @@ module subroutine symba_util_sort_tp(self, sortby, ascending) end if associate(tp => self, ntp => self%nbody) + allocate(ind(ntp)) select case(sortby) case("nplenc") call util_sort(direction * tp%nplenc(1:ntp), ind(1:ntp)) @@ -625,6 +758,35 @@ module subroutine symba_util_sort_tp(self, sortby, ascending) end subroutine symba_util_sort_tp + + module subroutine symba_util_sort_rearrange_arr_kin(arr, ind, n) + !! author: David A. Minton + !! + !! Rearrange a single array of particle kinship type in-place from an index list. + implicit none + ! Arguments + type(symba_kinship), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange + ! Internals + type(symba_kinship), dimension(:), allocatable :: tmp !! Temporary copy of array used during rearrange operation + integer(I4B) :: i,j + + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, source=arr) + tmp(1:n) = arr(ind(1:n)) + + do i = 1, n + do j = 1, tmp(i)%nchild + tmp(i)%child(j) = ind(tmp(i)%child(j)) + end do + end do + + call move_alloc(tmp, arr) + return + end subroutine symba_util_sort_rearrange_arr_kin + + module subroutine symba_util_sort_rearrange_pl(self, ind) !! author: David A. Minton !! @@ -635,32 +797,22 @@ module subroutine symba_util_sort_rearrange_pl(self, ind) class(symba_pl), intent(inout) :: self !! SyMBA massive body object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) ! Internals - class(symba_pl), allocatable :: pl_sorted !! Temporary holder for sorted body integer(I4B) :: i, j associate(pl => self, npl => self%nbody) + call util_sort_rearrange(pl%lcollision, ind, npl) + call util_sort_rearrange(pl%lencounter, ind, npl) + call util_sort_rearrange(pl%lmtiny, ind, npl) + call util_sort_rearrange(pl%nplenc, ind, npl) + call util_sort_rearrange(pl%ntpenc, ind, npl) + call util_sort_rearrange(pl%levelg, ind, npl) + call util_sort_rearrange(pl%levelm, ind, npl) + call util_sort_rearrange(pl%isperi, ind, npl) + call util_sort_rearrange(pl%peri, ind, npl) + call util_sort_rearrange(pl%atp, ind, npl) + call util_sort_rearrange(pl%kin, ind, npl) + call util_sort_rearrange_pl(pl,ind) - allocate(pl_sorted, source=self) - if (allocated(pl%lcollision)) pl%lcollision(1:npl) = pl_sorted%lcollision(ind(1:npl)) - if (allocated(pl%lencounter)) pl%lencounter(1:npl) = pl_sorted%lencounter(ind(1:npl)) - if (allocated(pl%lmtiny)) pl%lmtiny(1:npl) = pl_sorted%lmtiny(ind(1:npl)) - if (allocated(pl%nplenc)) pl%nplenc(1:npl) = pl_sorted%nplenc(ind(1:npl)) - if (allocated(pl%ntpenc)) pl%ntpenc(1:npl) = pl_sorted%ntpenc(ind(1:npl)) - if (allocated(pl%levelg)) pl%levelg(1:npl) = pl_sorted%levelg(ind(1:npl)) - if (allocated(pl%levelm)) pl%levelm(1:npl) = pl_sorted%levelm(ind(1:npl)) - if (allocated(pl%isperi)) pl%isperi(1:npl) = pl_sorted%isperi(ind(1:npl)) - if (allocated(pl%peri)) pl%peri(1:npl) = pl_sorted%peri(ind(1:npl)) - if (allocated(pl%atp)) pl%atp(1:npl) = pl_sorted%atp(ind(1:npl)) - if (allocated(pl%info)) pl%info(1:npl) = pl_sorted%info(ind(1:npl)) - if (allocated(pl%kin)) then - pl%kin(1:npl) = pl_sorted%kin(ind(1:npl)) - do i = 1, npl - do j = 1, pl%kin(i)%nchild - pl%kin(i)%child(j) = ind(pl%kin(i)%child(j)) - end do - end do - end if - deallocate(pl_sorted) end associate return @@ -676,51 +828,19 @@ module subroutine symba_util_sort_rearrange_tp(self, ind) ! Arguments class(symba_tp), intent(inout) :: self !! SyMBA test particle object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - ! Internals - class(symba_tp), allocatable :: tp_sorted !! Temporary holder for sorted body associate(tp => self, ntp => self%nbody) + call util_sort_rearrange(tp%nplenc, ind, ntp) + call util_sort_rearrange(tp%levelg, ind, ntp) + call util_sort_rearrange(tp%levelm, ind, ntp) + call util_sort_rearrange_tp(tp,ind) - allocate(tp_sorted, source=self) - if (allocated(tp%nplenc)) tp%nplenc(1:ntp) = tp_sorted%nplenc(ind(1:ntp)) - if (allocated(tp%levelg)) tp%levelg(1:ntp) = tp_sorted%levelg(ind(1:ntp)) - if (allocated(tp%levelm)) tp%levelm(1:ntp) = tp_sorted%levelm(ind(1:ntp)) - if (allocated(tp%info)) tp%info(1:ntp) = tp_sorted%info(ind(1:ntp)) - deallocate(tp_sorted) end associate return end subroutine symba_util_sort_rearrange_tp - module subroutine symba_util_spill_arr_info(keeps, discards, lspill_list, ldestructive) - !! author: David A. Minton - !! - !! Performs a spill operation on a single array of particle origin information types - !! This is the inverse of a spill operation - implicit none - ! Arguments - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep - type(symba_particle_info), dimension(:), allocatable, intent(inout) :: discards !! Array of discards - logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss - logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not - - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) - if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) - else - deallocate(keeps) - end if - end if - - return - end subroutine symba_util_spill_arr_info - - module subroutine symba_util_spill_arr_kin(keeps, discards, lspill_list, ldestructive) !! author: David A. Minton !! @@ -732,14 +852,25 @@ module subroutine symba_util_spill_arr_kin(keeps, discards, lspill_list, ldestru type(symba_kinship), dimension(:), allocatable, intent(inout) :: discards !! Array of discards logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: nspill, nkeep, nlist + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) + if (nkeep > 0) then + keeps(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) else deallocate(keeps) end if @@ -760,8 +891,6 @@ module subroutine symba_util_spill_pl(self, discards, lspill_list, ldestructive) class(swiftest_body), intent(inout) :: discards !! Discarded object logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list - ! Internals - integer(I4B) :: i ! For each component, pack the discarded bodies into the discard object and do the inverse with the keeps !> Spill all the common components @@ -778,7 +907,6 @@ module subroutine symba_util_spill_pl(self, discards, lspill_list, ldestructive) call util_spill(keeps%isperi, discards%isperi, lspill_list, ldestructive) call util_spill(keeps%peri, discards%peri, lspill_list, ldestructive) call util_spill(keeps%atp, discards%atp, lspill_list, ldestructive) - call util_spill(keeps%info, discards%info, lspill_list, ldestructive) call util_spill(keeps%kin, discards%kin, lspill_list, ldestructive) call util_spill_pl(keeps, discards, lspill_list, ldestructive) @@ -792,33 +920,31 @@ module subroutine symba_util_spill_pl(self, discards, lspill_list, ldestructive) end subroutine symba_util_spill_pl - module subroutine symba_util_spill_pltpenc(self, discards, lspill_list, ldestructive) + module subroutine symba_util_spill_encounter(self, discards, lspill_list, ldestructive) !! author: David A. Minton !! !! Move spilled (discarded) SyMBA encounter structure from active list to discard list !! Note: Because the symba_plplenc currently does not contain any additional variable components, this method can recieve it as an input as well. implicit none ! Arguments - class(symba_pltpenc), intent(inout) :: self !! SyMBA pl-tp encounter list + class(symba_encounter), intent(inout) :: self !! SyMBA pl-tp encounter list class(swiftest_encounter), intent(inout) :: discards !! Discarded object logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list - ! Internals - integer(I4B) :: i associate(keeps => self) select type(discards) - class is (symba_pltpenc) + class is (symba_encounter) call util_spill(keeps%level, discards%level, lspill_list, ldestructive) call util_spill_encounter(keeps, discards, lspill_list, ldestructive) class default - write(*,*) "Invalid object passed to the spill method. Source must be of class symba_pltpenc or its descendents!" + write(*,*) "Invalid object passed to the spill method. Source must be of class symba_encounter or its descendents!" call util_exit(FAILURE) end select end associate return - end subroutine symba_util_spill_pltpenc + end subroutine symba_util_spill_encounter module subroutine symba_util_spill_tp(self, discards, lspill_list, ldestructive) @@ -832,8 +958,6 @@ module subroutine symba_util_spill_tp(self, discards, lspill_list, ldestructive) class(swiftest_body), intent(inout) :: discards !! Discarded object logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list - ! Internals - integer(I4B) :: i ! For each component, pack the discarded bodies into the discard object and do the inverse with the keeps !> Spill all the common components @@ -843,7 +967,6 @@ module subroutine symba_util_spill_tp(self, discards, lspill_list, ldestructive) call util_spill(keeps%nplenc, discards%nplenc, lspill_list, ldestructive) call util_spill(keeps%levelg, discards%levelg, lspill_list, ldestructive) call util_spill(keeps%levelm, discards%levelm, lspill_list, ldestructive) - call util_spill(keeps%info, discards%info, lspill_list, ldestructive) call util_spill_tp(keeps, discards, lspill_list, ldestructive) class default @@ -855,4 +978,4 @@ module subroutine symba_util_spill_tp(self, discards, lspill_list, ldestructive) return end subroutine symba_util_spill_tp -end submodule s_symba_util \ No newline at end of file +end submodule s_symba_util diff --git a/src/tides/tides_getacch_pl.f90 b/src/tides/tides_getacch_pl.f90 index f0bf64cc7..4feb76221 100644 --- a/src/tides/tides_getacch_pl.f90 +++ b/src/tides/tides_getacch_pl.f90 @@ -48,8 +48,8 @@ module subroutine tides_kick_getacch_pl(self, system) Ftr = -3 / rmag**7 * (r5cbterm + r5plterm) - 3 * vmag / rmag * (Ptocb + Ptopl) F_T(:) = (Ftr + (Ptocb + Ptopl) * dot_product(v_unit, r_unit) / rmag) * r_unit(:) & - + Ptopl * (pl%rot(:,i) - theta_dot(:)) .cross. r_unit(:) & - + Ptocb * (cb%rot(:) - theta_dot(:)) .cross. r_unit(:) + + Ptopl * ((pl%rot(:,i) - theta_dot(:)) .cross. r_unit(:)) & + + Ptocb * ((cb%rot(:) - theta_dot(:)) .cross. r_unit(:)) cb%atide(:) = cb%atide(:) + F_T(:) / cb%Gmass pl%atide(:,i) = F_T(:) / pl%Gmass(i) end do diff --git a/src/util/util_append.f90 b/src/util/util_append.f90 index dc48f9861..ffe576c85 100644 --- a/src/util/util_append.f90 +++ b/src/util/util_append.f90 @@ -12,16 +12,19 @@ module subroutine util_append_arr_char_string(arr, source, nold, nsrc, lsource_m character(len=STRMAX), dimension(:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) + allocate(arr(nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) + arr(nold + 1:nold + nnew) = pack(source(1:nsrc), lsource_mask(1:nsrc)) return end subroutine util_append_arr_char_string @@ -37,16 +40,19 @@ module subroutine util_append_arr_DP(arr, source, nold, nsrc, lsource_mask) real(DP), dimension(:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) + allocate(arr(nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) + arr(nold + 1:nold + nnew) = pack(source(1:nsrc), lsource_mask(1:nsrc)) return end subroutine util_append_arr_DP @@ -62,18 +68,21 @@ module subroutine util_append_arr_DPvec(arr, source, nold, nsrc, lsource_mask) real(DP), dimension(:,:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(NDIM, nold+nsrc)) + allocate(arr(NDIM,nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(1, nold + 1:nold + nsrc) = pack(source(1,1:nsrc), lsource_mask(1:nsrc)) - arr(2, nold + 1:nold + nsrc) = pack(source(2,1:nsrc), lsource_mask(1:nsrc)) - arr(3, nold + 1:nold + nsrc) = pack(source(3,1:nsrc), lsource_mask(1:nsrc)) + arr(1, nold + 1:nold + nnew) = pack(source(1,1:nsrc), lsource_mask(1:nsrc)) + arr(2, nold + 1:nold + nnew) = pack(source(2,1:nsrc), lsource_mask(1:nsrc)) + arr(3, nold + 1:nold + nnew) = pack(source(3,1:nsrc), lsource_mask(1:nsrc)) return end subroutine util_append_arr_DPvec @@ -89,21 +98,57 @@ module subroutine util_append_arr_I4B(arr, source, nold, nsrc, lsource_mask) integer(I4B), dimension(:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) + allocate(arr(nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) + arr(nold + 1:nold + nnew) = pack(source(1:nsrc), lsource_mask(1:nsrc)) return end subroutine util_append_arr_I4B + module subroutine util_append_arr_info(arr, source, nold, nsrc, lsource_mask) + !! author: David A. Minton + !! + !! Append a single array of particle information type onto another. If the destination array is not allocated, or is not big enough, this will allocate space for it. + implicit none + ! Arguments + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array + type(swiftest_particle_info), dimension(:), allocatable, intent(in) :: source !! Array to append + integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew, i + integer(I4B), dimension(:), allocatable :: idx + + if (.not. allocated(source)) return + + nnew = count(lsource_mask(1:nsrc)) + if (.not.allocated(arr)) then + allocate(arr(nold+nnew)) + else + call util_resize(arr, nold + nnew) + end if + + allocate(idx(nnew)) + + idx = pack([(i, i = 1, nsrc)], lsource_mask(1:nsrc)) + + call util_copy_particle_info_arr(source(1:nsrc), arr(nold+1:nold+nnew), idx) + + return + end subroutine util_append_arr_info + + module subroutine util_append_arr_logical(arr, source, nold, nsrc, lsource_mask) !! author: David A. Minton !! @@ -114,16 +159,19 @@ module subroutine util_append_arr_logical(arr, source, nold, nsrc, lsource_mask) logical, dimension(:), allocatable, intent(in) :: source !! Array to append integer(I4B), intent(in) :: nold, nsrc !! Extend of the old array and the source array, respectively logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nnew if (.not. allocated(source)) return + nnew = count(lsource_mask(1:nsrc)) if (.not.allocated(arr)) then - allocate(arr(nold+nsrc)) + allocate(arr(nold+nnew)) else - call util_resize(arr, nold + nsrc) + call util_resize(arr, nold + nnew) end if - arr(nold + 1:nold + nsrc) = pack(source(1:nsrc), lsource_mask(1:nsrc)) + arr(nold + 1:nold + nnew) = pack(source(1:nsrc), lsource_mask(1:nsrc)) return end subroutine util_append_arr_logical @@ -136,40 +184,76 @@ module subroutine util_append_body(self, source, lsource_mask) !! This method will automatically resize the destination body if it is too small implicit none ! Arguments - class(swiftest_body), intent(inout) :: self !! Swiftest body object - class(swiftest_body), intent(in) :: source !! Source object to append - logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to - - associate(nold => self%nbody, nsrc => source%nbody) - call util_append(self%name, source%name, nold, nsrc, lsource_mask) - call util_append(self%id, source%id, nold, nsrc, lsource_mask) - call util_append(self%status, source%status, nold, nsrc, lsource_mask) - call util_append(self%ldiscard, source%ldiscard, nold, nsrc, lsource_mask) - call util_append(self%lmask, source%lmask, nold, nsrc, lsource_mask) - call util_append(self%mu, source%mu, nold, nsrc, lsource_mask) - call util_append(self%xh, source%xh, nold, nsrc, lsource_mask) - call util_append(self%vh, source%vh, nold, nsrc, lsource_mask) - call util_append(self%xb, source%xb, nold, nsrc, lsource_mask) - call util_append(self%vb, source%vb, nold, nsrc, lsource_mask) - call util_append(self%ah, source%ah, nold, nsrc, lsource_mask) - call util_append(self%aobl, source%aobl, nold, nsrc, lsource_mask) - call util_append(self%atide, source%atide, nold, nsrc, lsource_mask) - call util_append(self%agr, source%agr, nold, nsrc, lsource_mask) - call util_append(self%ir3h, source%ir3h, nold, nsrc, lsource_mask) - call util_append(self%a, source%a, nold, nsrc, lsource_mask) - call util_append(self%e, source%e, nold, nsrc, lsource_mask) - call util_append(self%inc, source%inc, nold, nsrc, lsource_mask) - call util_append(self%capom, source%capom, nold, nsrc, lsource_mask) - call util_append(self%omega, source%omega, nold, nsrc, lsource_mask) - call util_append(self%capm, source%capm, nold, nsrc, lsource_mask) - end associate - - self%nbody = count(self%status(:) /= INACTIVE) + class(swiftest_body), intent(inout) :: self !! Swiftest body object + class(swiftest_body), intent(in) :: source !! Source object to append + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nold, nsrc, nnew + + nold = self%nbody + nsrc = source%nbody + nnew = count(lsource_mask(1:nsrc)) + + call util_append(self%info, source%info, nold, nsrc, lsource_mask) + call util_append(self%id, source%id, nold, nsrc, lsource_mask) + call util_append(self%status, source%status, nold, nsrc, lsource_mask) + call util_append(self%ldiscard, source%ldiscard, nold, nsrc, lsource_mask) + call util_append(self%lmask, source%lmask, nold, nsrc, lsource_mask) + call util_append(self%mu, source%mu, nold, nsrc, lsource_mask) + call util_append(self%xh, source%xh, nold, nsrc, lsource_mask) + call util_append(self%vh, source%vh, nold, nsrc, lsource_mask) + call util_append(self%xb, source%xb, nold, nsrc, lsource_mask) + call util_append(self%vb, source%vb, nold, nsrc, lsource_mask) + call util_append(self%ah, source%ah, nold, nsrc, lsource_mask) + call util_append(self%aobl, source%aobl, nold, nsrc, lsource_mask) + call util_append(self%atide, source%atide, nold, nsrc, lsource_mask) + call util_append(self%agr, source%agr, nold, nsrc, lsource_mask) + call util_append(self%ir3h, source%ir3h, nold, nsrc, lsource_mask) + call util_append(self%a, source%a, nold, nsrc, lsource_mask) + call util_append(self%e, source%e, nold, nsrc, lsource_mask) + call util_append(self%inc, source%inc, nold, nsrc, lsource_mask) + call util_append(self%capom, source%capom, nold, nsrc, lsource_mask) + call util_append(self%omega, source%omega, nold, nsrc, lsource_mask) + call util_append(self%capm, source%capm, nold, nsrc, lsource_mask) + + self%nbody = nold + nnew return end subroutine util_append_body + module subroutine util_append_encounter(self, source, lsource_mask) + !! author: David A. Minton + !! + !! Append components from one Swiftest body object to another. + !! This method will automatically resize the destination body if it is too small + implicit none + ! Arguments + class(swiftest_encounter), intent(inout) :: self !! Swiftest encounter list object + class(swiftest_encounter), intent(in) :: source !! Source object to append + logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to + ! Internals + integer(I4B) :: nold, nsrc + + nold = self%nenc + nsrc = source%nenc + call util_append(self%lvdotr, source%lvdotr, nold, nsrc, lsource_mask) + call util_append(self%status, source%status, nold, nsrc, lsource_mask) + call util_append(self%index1, source%index1, nold, nsrc, lsource_mask) + call util_append(self%index2, source%index2, nold, nsrc, lsource_mask) + call util_append(self%id1, source%id1, nold, nsrc, lsource_mask) + call util_append(self%id2, source%id2, nold, nsrc, lsource_mask) + call util_append(self%x1, source%x1, nold, nsrc, lsource_mask) + call util_append(self%x2, source%x2, nold, nsrc, lsource_mask) + call util_append(self%v1, source%v1, nold, nsrc, lsource_mask) + call util_append(self%v2, source%v2, nold, nsrc, lsource_mask) + call util_append(self%t, source%t, nold, nsrc, lsource_mask) + self%nenc = nold + count(lsource_mask(1:nsrc)) + + return + end subroutine util_append_encounter + + module subroutine util_append_pl(self, source, lsource_mask) !! author: David A. Minton !! @@ -181,7 +265,6 @@ module subroutine util_append_pl(self, source, lsource_mask) class(swiftest_body), intent(in) :: source !! Source object to append logical, dimension(:), intent(in) :: lsource_mask !! Logical mask indicating which elements to append to - select type(source) class is (swiftest_pl) associate(nold => self%nbody, nsrc => source%nbody) @@ -199,10 +282,10 @@ module subroutine util_append_pl(self, source, lsource_mask) call util_append(self%Q, source%Q, nold, nsrc, lsource_mask) call util_append(self%tlag, source%tlag, nold, nsrc, lsource_mask) + if (allocated(self%k_plpl)) deallocate(self%k_plpl) + call util_append_body(self, source, lsource_mask) end associate - - call self%eucl_index() class default write(*,*) "Invalid object passed to the append method. Source must be of class swiftest_pl or its descendents" call util_exit(FAILURE) diff --git a/src/util/util_coord.f90 b/src/util/util_coord.f90 index 2a970d0dc..b4a77231c 100644 --- a/src/util/util_coord.f90 +++ b/src/util/util_coord.f90 @@ -45,7 +45,7 @@ end subroutine util_coord_h2b_pl module subroutine util_coord_h2b_tp(self, cb) !! author: David A. Minton !! - !! Convert massive bodies from heliocentric to barycentric coordinates (position and velocity) + !! Convert test particles from heliocentric to barycentric coordinates (position and velocity) !! !! Adapted from David E. Kaufmann's Swifter routine coord_h2b_tp.f90 !! Adapted from Hal Levison's Swift routine coord_h2b_tp.f @@ -120,5 +120,174 @@ module subroutine util_coord_b2h_tp(self, cb) return end subroutine util_coord_b2h_tp + + + module subroutine util_coord_vb2vh_pl(self, cb) + !! author: David A. Minton + !! + !! Convert massive bodies from barycentric to heliocentric coordinates (velocity only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_vb2vh.f90 + !! Adapted from Hal Levison's Swift routine coord_vb2vh.f + implicit none + ! Arguments + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + ! Internals + integer(I4B) :: i + + if (self%nbody == 0) return + + associate(pl => self, npl => self%nbody) + do i = 1, NDIM + cb%vb(i) = -sum(pl%Gmass(1:npl) * pl%vb(i, 1:npl)) / cb%Gmass + pl%vh(i, 1:npl) = pl%vb(i, 1:npl) - cb%vb(i) + end do + end associate + + return + end subroutine util_coord_vb2vh_pl + + + module subroutine util_coord_vb2vh_tp(self, vbcb) + !! author: David A. Minton + !! + !! Convert test particles from barycentric to heliocentric coordinates (velocity only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_vb2vh_tp.f90 + !! Adapted from Hal Levison's Swift routine coord_vb2h_tp.f + implicit none + ! Arguments + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body + + if (self%nbody == 0) return + + associate(tp => self, ntp => self%nbody) + where (tp%lmask(1:ntp)) + tp%vh(1, 1:ntp) = tp%vb(1, 1:ntp) - vbcb(1) + tp%vh(2, 1:ntp) = tp%vb(2, 1:ntp) - vbcb(2) + tp%vh(3, 1:ntp) = tp%vb(3, 1:ntp) - vbcb(3) + end where + end associate + + return + end subroutine util_coord_vb2vh_tp + + + module subroutine util_coord_vh2vb_pl(self, cb) + !! author: David A. Minton + !! + !! Convert massive bodies from heliocentric to barycentric coordinates (velocity only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_vh2vb.f90 + !! Adapted from Hal Levison's Swift routine coord_vh2b.f + implicit none + ! Arguments + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + ! Internals + integer(I4B) :: i + real(DP) :: Gmtot + + if (self%nbody == 0) return + + associate(pl => self, npl => self%nbody) + Gmtot = cb%Gmass + sum(pl%Gmass(1:npl)) + do i = 1, NDIM + cb%vb(i) = -sum(pl%Gmass(1:npl) * pl%vh(i, 1:npl)) / Gmtot + pl%vb(i, 1:npl) = pl%vh(i, 1:npl) + cb%vb(i) + end do + end associate + + return + end subroutine util_coord_vh2vb_pl + + + module subroutine util_coord_vh2vb_tp(self, vbcb) + !! author: David A. Minton + !! + !! Convert test particles from heliocentric to barycentric coordinates (velocity only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_vh2vb_tp.f90 + !! Adapted from Hal Levison's Swift routine coord_vh2b_tp.f + implicit none + ! Arguments + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + real(DP), dimension(:), intent(in) :: vbcb !! Barycentric velocity of the central body + + if (self%nbody == 0) return + + associate(tp => self, ntp => self%nbody) + where (tp%lmask(1:ntp)) + tp%vb(1, 1:ntp) = tp%vh(1, 1:ntp) + vbcb(1) + tp%vb(2, 1:ntp) = tp%vh(2, 1:ntp) + vbcb(2) + tp%vb(3, 1:ntp) = tp%vh(3, 1:ntp) + vbcb(3) + end where + end associate + + return + end subroutine util_coord_vh2vb_tp + + module subroutine util_coord_xh2xb_pl(self, cb) + !! author: David A. Minton + !! + !! Convert position vectors of massive bodies from heliocentric to barycentric coordinates (position only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_h2b.f90 + !! Adapted from Hal Levison's Swift routine coord_h2b.f + implicit none + ! Arguments + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object + ! Internals + integer(I4B) :: i + real(DP) :: Gmtot + real(DP), dimension(NDIM) :: xtmp + + if (self%nbody == 0) return + associate(pl => self, npl => self%nbody) + Gmtot = cb%Gmass + xtmp(:) = 0.0_DP + do i = 1, npl + if (pl%status(i) == INACTIVE) cycle + Gmtot = Gmtot + pl%Gmass(i) + xtmp(:) = xtmp(:) + pl%Gmass(i) * pl%xh(:,i) + end do + cb%xb(:) = -xtmp(:) / Gmtot + do i = 1, npl + if (pl%status(i) == INACTIVE) cycle + pl%xb(:,i) = pl%xh(:,i) + cb%xb(:) + end do + end associate + + return + end subroutine util_coord_xh2xb_pl + + + module subroutine util_coord_xh2xb_tp(self, cb) + !! author: David A. Minton + !! + !! Convert test particles from heliocentric to barycentric coordinates (position only) + !! + !! Adapted from David E. Kaufmann's Swifter routine coord_h2b_tp.f90 + !! Adapted from Hal Levison's Swift routine coord_h2b_tp.f + implicit none + ! Arguments + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + class(swiftest_cb), intent(in) :: cb !! Swiftest central body object + ! Internals + integer(I4B) :: i + + if (self%nbody == 0) return + associate(tp => self, ntp => self%nbody) + do concurrent (i = 1:ntp, tp%status(i) /= INACTIVE) + tp%xb(:, i) = tp%xh(:, i) + cb%xb(:) + end do + end associate + + return + end subroutine util_coord_xh2xb_tp + end submodule s_util_coord \ No newline at end of file diff --git a/src/util/util_copy.f90 b/src/util/util_copy.f90 index f44777eec..60d93e45e 100644 --- a/src/util/util_copy.f90 +++ b/src/util/util_copy.f90 @@ -2,28 +2,100 @@ use swiftest contains -module subroutine util_copy_encounter(self, source) - !! author: David A. Minton - !! - !! Copies elements from the source encounter list into self. - implicit none - ! Arguments - class(swiftest_encounter), intent(inout) :: self !! Encounter list - class(swiftest_encounter), intent(in) :: source !! Source object to copy into - - associate(n => source%nenc) - self%nenc = n - self%lvdotr(1:n) = source%lvdotr(1:n) - self%status(1:n) = source%status(1:n) - self%index1(1:n) = source%index1(1:n) - self%index2(1:n) = source%index2(1:n) - self%x1(:,1:n) = source%x1(:,1:n) - self%x2(:,1:n) = source%x2(:,1:n) - self%v1(:,1:n) = source%v1(:,1:n) - self%v2(:,1:n) = source%v2(:,1:n) - end associate - - return -end subroutine util_copy_encounter + module subroutine util_copy_encounter(self, source) + !! author: David A. Minton + !! + !! Copies elements from the source encounter list into self. + implicit none + ! Arguments + class(swiftest_encounter), intent(inout) :: self !! Encounter list + class(swiftest_encounter), intent(in) :: source !! Source object to copy into + + associate(n => source%nenc) + self%nenc = n + self%lvdotr(1:n) = source%lvdotr(1:n) + self%status(1:n) = source%status(1:n) + self%kidx(1:n) = source%kidx(1:n) + self%index1(1:n) = source%index1(1:n) + self%index2(1:n) = source%index2(1:n) + self%id1(1:n) = source%id1(1:n) + self%id2(1:n) = source%id2(1:n) + self%x1(:,1:n) = source%x1(:,1:n) + self%x2(:,1:n) = source%x2(:,1:n) + self%v1(:,1:n) = source%v1(:,1:n) + self%v2(:,1:n) = source%v2(:,1:n) + self%t(1:n) = source%t(1:n) + end associate + + return + end subroutine util_copy_encounter + + + module subroutine util_copy_particle_info(self, source) + !! author: David A. Minton + !! + !! Copies one set of information object components into another, component-by-component + implicit none + class(swiftest_particle_info), intent(inout) :: self + class(swiftest_particle_info), intent(in) :: source + + call self%set_value(& + name = source%name, & + particle_type = source%particle_type, & + status = source%status, & + origin_type = source%origin_type, & + origin_time = source%origin_time, & + origin_xh = source%origin_xh(:), & + origin_vh = source%origin_vh(:), & + discard_time = source%discard_time, & + discard_xh = source%discard_xh(:), & + discard_vh = source%discard_vh(:), & + discard_body_id = source%discard_body_id & + ) + + return + end subroutine util_copy_particle_info + + + module subroutine util_copy_particle_info_arr(source, dest, idx) + !! author: David A. Minton + !! + !! Copies contents from an array of one particle information objects to another. + implicit none + class(swiftest_particle_info), dimension(:), intent(in) :: source !! Source object to copy into + class(swiftest_particle_info), dimension(:), intent(inout) :: dest !! Swiftest body object with particle metadata information object + integer(I4B), dimension(:), intent(in), optional :: idx !! Optional array of indices to draw the source object + ! Internals + integer(I4B) :: i, j, n, nsource, ndest + + if (size(source) == 0) return + + if (present(idx)) then + n = size(idx) + else + n = size(source) + end if + + nsource = size(source) + ndest = size(dest) + + if ((n == 0) .or. (n > ndest) .or. (n > nsource)) then + write(*,*) 'Particle info copy operation failed. n, nsource, ndest: ',n, nsource, ndest + return + end if + + do i = 1, n + if (present(idx)) then + j = idx(i) + else + j = i + end if + call dest(i)%copy(source(j)) + end do + + return + end subroutine util_copy_particle_info_arr + + end submodule s_util_copy diff --git a/src/util/util_fill.f90 b/src/util/util_fill.f90 index 4a5a70311..26b21310e 100644 --- a/src/util/util_fill.f90 +++ b/src/util/util_fill.f90 @@ -82,6 +82,35 @@ module subroutine util_fill_arr_I4B(keeps, inserts, lfill_list) return end subroutine util_fill_arr_I4B + + module subroutine util_fill_arr_info(keeps, inserts, lfill_list) + !! author: David A. Minton + !! + !! Performs a fill operation on a single array of particle origin information types + !! This is the inverse of a spill operation + implicit none + ! Arguments + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + type(swiftest_particle_info), dimension(:), allocatable, intent(in) :: inserts !! Array of values to insert into keep + logical, dimension(:), intent(in) :: lfill_list !! Logical array of bodies to merge into the keeps + ! Internals + integer(I4B), dimension(:), allocatable :: insert_idx + integer(I4B) :: i, nkeep, ninsert + + if (.not.allocated(keeps) .or. .not.allocated(inserts)) return + + nkeep = size(keeps) + ninsert = count(lfill_list) + + allocate(insert_idx(ninsert)) + + insert_idx(:) = pack([(i, i = 1, nkeep)], lfill_list) + call util_copy_particle_info_arr(inserts, keeps, insert_idx) + + return + end subroutine util_fill_arr_info + + module subroutine util_fill_arr_logical(keeps, inserts, lfill_list) !! author: David A. Minton !! @@ -119,7 +148,7 @@ module subroutine util_fill_body(self, inserts, lfill_list) !> Fill all the common components associate(keeps => self) call util_fill(keeps%id, inserts%id, lfill_list) - call util_fill(keeps%name, inserts%name, lfill_list) + call util_fill(keeps%info, inserts%info, lfill_list) call util_fill(keeps%status, inserts%status, lfill_list) call util_fill(keeps%ldiscard, inserts%ldiscard, lfill_list) call util_fill(keeps%lmask, inserts%lmask, lfill_list) @@ -177,6 +206,8 @@ module subroutine util_fill_pl(self, inserts, lfill_list) call util_fill(keeps%vbeg, inserts%vbeg, lfill_list) call util_fill(keeps%Ip, inserts%Ip, lfill_list) call util_fill(keeps%rot, inserts%rot, lfill_list) + + if (allocated(keeps%k_plpl)) deallocate(keeps%k_plpl) call util_fill_body(keeps, inserts, lfill_list) class default diff --git a/src/util/util_get_energy_momentum.f90 b/src/util/util_get_energy_momentum.f90 index fa7cda43d..803b7bac1 100644 --- a/src/util/util_get_energy_momentum.f90 +++ b/src/util/util_get_energy_momentum.f90 @@ -14,19 +14,21 @@ module subroutine util_get_energy_momentum_system(self, param) class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters ! Internals integer(I4B) :: i, j - integer(I8B) :: k + integer(I8B) :: k, nplpl real(DP) :: oblpot, kecb, kespincb real(DP), dimension(self%pl%nbody) :: irh, kepl, kespinpl, pecb real(DP), dimension(self%pl%nbody) :: Lplorbitx, Lplorbity, Lplorbitz real(DP), dimension(self%pl%nbody) :: Lplspinx, Lplspiny, Lplspinz - real(DP), dimension(self%pl%nplpl) :: pepl real(DP), dimension(NDIM) :: Lcborbit, Lcbspin - logical, dimension(self%pl%nplpl) :: lstatpl - logical, dimension(self%pl%nbody) :: lstatus + real(DP), dimension(:), allocatable :: pepl + logical, dimension(:), allocatable :: lstatpl + real(DP) :: hx, hy, hz associate(system => self, pl => self%pl, npl => self%pl%nbody, cb => self%cb) + nplpl = pl%nplpl system%Lorbit(:) = 0.0_DP system%Lspin(:) = 0.0_DP + system%Ltot(:) = 0.0_DP system%ke_orbit = 0.0_DP system%ke_spin = 0.0_DP @@ -37,27 +39,25 @@ module subroutine util_get_energy_momentum_system(self, param) Lplspinx(:) = 0.0_DP Lplspiny(:) = 0.0_DP Lplspinz(:) = 0.0_DP - lstatus(1:npl) = pl%status(1:npl) /= INACTIVE + pl%lmask(1:npl) = pl%status(1:npl) /= INACTIVE + + system%GMtot = cb%Gmass + sum(pl%Gmass(1:npl), pl%lmask(1:npl)) kecb = cb%mass * dot_product(cb%vb(:), cb%vb(:)) - Lcborbit(:) = cb%mass * cb%xb(:) .cross. cb%vb(:) - - do concurrent (i = 1:npl, lstatus(i)) - block ! We use a block construct to prevent generating temporary arrays for local variables - real(DP) :: v2, hx, hy, hz - v2 = dot_product(pl%vb(:,i), pl%vb(:,i)) - hx = pl%xb(2,i) * pl%vb(3,i) - pl%xb(3,i) * pl%vb(2,i) - hy = pl%xb(3,i) * pl%vb(1,i) - pl%xb(1,i) * pl%vb(3,i) - hz = pl%xb(1,i) * pl%vb(2,i) - pl%xb(2,i) * pl%vb(1,i) - - ! Angular momentum from orbit - Lplorbitx(i) = pl%mass(i) * hx - Lplorbity(i) = pl%mass(i) * hy - Lplorbitz(i) = pl%mass(i) * hz - - ! Kinetic energy from orbit and spin - kepl(i) = pl%mass(i) * v2 - end block + Lcborbit(:) = cb%mass * (cb%xb(:) .cross. cb%vb(:)) + + do concurrent (i = 1:npl, pl%lmask(i)) + hx = pl%xb(2,i) * pl%vb(3,i) - pl%xb(3,i) * pl%vb(2,i) + hy = pl%xb(3,i) * pl%vb(1,i) - pl%xb(1,i) * pl%vb(3,i) + hz = pl%xb(1,i) * pl%vb(2,i) - pl%xb(2,i) * pl%vb(1,i) + + ! Angular momentum from orbit + Lplorbitx(i) = pl%mass(i) * hx + Lplorbity(i) = pl%mass(i) * hy + Lplorbitz(i) = pl%mass(i) * hz + + ! Kinetic energy from orbit + kepl(i) = pl%mass(i) * dot_product(pl%vb(:,i), pl%vb(:,i)) end do if (param%lrotation) then @@ -66,22 +66,15 @@ module subroutine util_get_energy_momentum_system(self, param) ! For simplicity, we always assume that the rotation pole is the 3rd principal axis Lcbspin(:) = cb%Ip(3) * cb%mass * cb%radius**2 * cb%rot(:) - do concurrent (i = 1:npl, lstatus(i)) - block - real(DP) :: rot2, hsx, hsy, hsz + do concurrent (i = 1:npl, pl%lmask(i)) + ! Currently we assume that the rotation pole is the 3rd principal axis + ! Angular momentum from spin + Lplspinx(i) = pl%mass(i) * pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(1,i) + Lplspiny(i) = pl%mass(i) * pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(2,i) + Lplspinz(i) = pl%mass(i) * pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(3,i) - rot2 = dot_product(pl%rot(:,i), pl%rot(:,i)) - ! For simplicity, we always assume that the rotation pole is the 3rd principal axis - hsx = pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(1,i) - hsy = pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(2,i) - hsz = pl%Ip(3,i) * pl%radius(i)**2 * pl%rot(3,i) - - ! Angular momentum from spin - Lplspinx(i) = pl%mass(i) * hsx - Lplspiny(i) = pl%mass(i) * hsy - Lplspinz(i) = pl%mass(i) * hsz - kespinpl(i) = pl%mass(i) * pl%Ip(3, i) * pl%radius(i)**2 * rot2 - end block + ! Kinetic energy from spin + kespinpl(i) = pl%mass(i) * pl%Ip(3,i) * pl%radius(i)**2 * dot_product(pl%rot(:,i), pl%rot(:,i)) end do else kespincb = 0.0_DP @@ -89,48 +82,57 @@ module subroutine util_get_energy_momentum_system(self, param) end if ! Do the central body potential energy component first - associate(px => pl%xb(1,:), py => pl%xb(2,:), pz => pl%xb(3,:)) - do concurrent(i = 1:npl, lstatus(i)) - pecb(i) = -cb%Gmass * pl%mass(i) / sqrt(px(i)**2 + py(i)**2 + pz(i)**2) - end do - end associate + where(.not. pl%lmask(1:npl)) + pecb(1:npl) = 0.0_DP + end where + + do concurrent(i = 1:npl, pl%lmask(i)) + pecb(i) = -cb%Gmass * pl%mass(i) / norm2(pl%xb(:,i)) + end do ! Do the potential energy between pairs of massive bodies - associate(indi => pl%k_plpl(1, :), indj => pl%k_plpl(2, :)) - do concurrent (k = 1:pl%nplpl) - lstatpl(k) = (lstatus(indi(k)) .and. lstatus(indj(k))) - end do + allocate(lstatpl(nplpl)) + allocate(pepl(nplpl)) + do concurrent (k = 1:nplpl) + i = pl%k_plpl(1,k) + j = pl%k_plpl(2,k) + lstatpl(k) = (pl%lmask(i) .and. pl%lmask(j)) + end do - do concurrent (k = 1:pl%nplpl, lstatpl(k)) - pepl(k) = -pl%Gmass(indi(k)) * pl%mass(indj(k)) / norm2(pl%xb(:, indi(k)) - pl%xb(:, indj(k))) - end do - end associate + where(.not.lstatpl(1:nplpl)) + pepl(1:nplpl) = 0.0_DP + end where + + do concurrent (k = 1:nplpl, lstatpl(k)) + i = pl%k_plpl(1,k) + j = pl%k_plpl(2,k) + pepl(k) = -(pl%Gmass(i) * pl%mass(j)) / norm2(pl%xb(:, i) - pl%xb(:, j)) + end do - system%pe = sum(pepl(:), lstatpl(:)) + sum(pecb(1:npl), lstatus(1:npl)) + system%pe = sum(pepl(:), lstatpl(:)) + sum(pecb(1:npl), pl%lmask(1:npl)) + deallocate(lstatpl, pepl) - system%ke_orbit = 0.5_DP * (kecb + sum(kepl(1:npl), lstatus(:))) - if (param%lrotation) system%ke_spin = 0.5_DP * (kespincb + sum(kespinpl(1:npl), lstatus(:))) + system%ke_orbit = 0.5_DP * (kecb + sum(kepl(1:npl), pl%lmask(1:npl))) + if (param%lrotation) system%ke_spin = 0.5_DP * (kespincb + sum(kespinpl(1:npl), pl%lmask(1:npl))) ! Potential energy from the oblateness term if (param%loblatecb) then - do concurrent(i = 1:npl, lstatus(i)) - irh(i) = 1.0_DP / norm2(pl%xh(:,i)) - end do - call obl_pot(npl, cb%Gmass, pl%mass, cb%j2rp2, cb%j4rp4, pl%xh, irh, oblpot) - system%pe = system%pe + oblpot + call system%obl_pot() + system%pe = system%pe + system%oblpot end if - system%Lorbit(1) = Lcborbit(1) + sum(Lplorbitx(1:npl), lstatus(1:npl)) - system%Lorbit(2) = Lcborbit(2) + sum(Lplorbity(1:npl), lstatus(1:npl)) - system%Lorbit(3) = Lcborbit(3) + sum(Lplorbitz(1:npl), lstatus(1:npl)) + system%Lorbit(1) = Lcborbit(1) + sum(Lplorbitx(1:npl), pl%lmask(1:npl)) + system%Lorbit(2) = Lcborbit(2) + sum(Lplorbity(1:npl), pl%lmask(1:npl)) + system%Lorbit(3) = Lcborbit(3) + sum(Lplorbitz(1:npl), pl%lmask(1:npl)) if (param%lrotation) then - system%Lspin(1) = Lcbspin(1) + sum(Lplspinx(1:npl), lstatus(1:npl)) - system%Lspin(2) = Lcbspin(2) + sum(Lplspiny(1:npl), lstatus(1:npl)) - system%Lspin(3) = Lcbspin(3) + sum(Lplspinz(1:npl), lstatus(1:npl)) + system%Lspin(1) = Lcbspin(1) + sum(Lplspinx(1:npl), pl%lmask(1:npl)) + system%Lspin(2) = Lcbspin(2) + sum(Lplspiny(1:npl), pl%lmask(1:npl)) + system%Lspin(3) = Lcbspin(3) + sum(Lplspinz(1:npl), pl%lmask(1:npl)) end if system%te = system%ke_orbit + system%ke_spin + system%pe + system%Ltot(:) = system%Lorbit(:) + system%Lspin(:) end associate return diff --git a/src/util/util_index.f90 b/src/util/util_index.f90 new file mode 100644 index 000000000..0e42ec7c7 --- /dev/null +++ b/src/util/util_index.f90 @@ -0,0 +1,76 @@ +submodule (swiftest_classes) s_util_index + use swiftest +contains + + module subroutine util_index_eucl_plpl(self, param) + !! author: Jacob R. Elliott and David A. Minton + !! + !! Turns i,j indices into k index for use in the Euclidean distance matrix for pl-pl interactions. + !! + !! Reference: + !! + !! Mélodie Angeletti, Jean-Marie Bonny, Jonas Koko. Parallel Euclidean distance matrix computation on big datasets *. + !! 2019. hal-0204751 + implicit none + ! Arguments + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I8B) :: i, j, counter, npl + + npl = int(self%nbody, kind=I8B) + associate(nplpl => self%nplpl) + nplpl = (npl * (npl - 1) / 2) ! number of entries in a strict lower triangle, npl x npl, minus first column + if (allocated(self%k_plpl)) deallocate(self%k_plpl) ! Reset the index array if it's been set previously + allocate(self%k_plpl(2, nplpl)) + do i = 1_I8B, npl + counter = (i - 1_I8B) * npl - i * (i - 1_I8B) / 2_I8B + 1_I8B + do j = i + 1_I8B, npl + self%k_plpl(1, counter) = i + self%k_plpl(2, counter) = j + counter = counter + 1_I8B + end do + end do + end associate + + return + end subroutine util_index_eucl_plpl + + + module subroutine util_index_eucl_pltp(self, pl, param) + !! author: Jacob R. Elliott and David A. Minton + !! + !! Turns i,j indices into k index for use in the Euclidean distance matrix for pl-tp interactions + !! + !! Reference: + !! + !! Mélodie Angeletti, Jean-Marie Bonny, Jonas Koko. Parallel Euclidean distance matrix computation on big datasets *. + !! 2019. hal-0204751 + implicit none + ! Arguments + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + class(swiftest_pl), intent(in) :: pl !! Swiftest massive body object + class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + ! Internals + integer(I8B) :: i, j, counter, npl, ntp + + ntp = int(self%nbody, kind=I8B) + npl = int(pl%nbody, kind=I8B) + associate(npltp => self%npltp) + npltp = npl * ntp + if (allocated(self%k_pltp)) deallocate(self%k_pltp) ! Reset the index array if it's been set previously + allocate(self%k_pltp(2, npltp)) + do i = 1_I8B, npl + counter = (i - 1_I8B) * npl + 1_I8B + do j = 1_I8B, ntp + self%k_pltp(1, counter) = i + self%k_pltp(2, counter) = j + counter = counter + 1_I8B + end do + end do + end associate + + return + end subroutine util_index_eucl_pltp + +end submodule s_util_index diff --git a/src/util/util_minimize_bfgs.f90 b/src/util/util_minimize_bfgs.f90 index fbd48c8c2..01b57d868 100644 --- a/src/util/util_minimize_bfgs.f90 +++ b/src/util/util_minimize_bfgs.f90 @@ -1,15 +1,16 @@ submodule (swiftest_classes) s_util_minimize_bfgs use swiftest contains - module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) + module function util_minimize_bfgs(f, N, x0, eps, maxloop, lerr) result(x1) !! author: David A. Minton !! - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - !! This function implements the Broyden-Fletcher-Goldfarb-Shanno method to determine the minimum of a function of N variables. !! It recieves as input: !! f%eval(x) : lambda function object containing the objective function as the eval metho - !! N : Number of variables of function f - !! x0 : Initial starting value of x - !! eps : Accuracy of 1 - dimensional minimization at each step + !! N : Number of variables of function f + !! x0 : Initial starting value of x + !! eps : Accuracy of 1 - dimensional minimization at each step + !! maxloop : Maximum number of loops to attempt to find a solution !! The outputs include !! lerr : Returns .true. if it could not find the minimum !! Returns @@ -23,12 +24,12 @@ module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) class(lambda_obj), intent(inout) :: f real(DP), dimension(:), intent(in) :: x0 real(DP), intent(in) :: eps + integer(I4B), intent(in) :: maxloop logical, intent(out) :: lerr ! Result real(DP), dimension(:), allocatable :: x1 ! Internals integer(I4B) :: i, j, k, l, conv, num - integer(I4B), parameter :: MAXLOOP = 1000 !! Maximum number of loops before method is determined to have failed real(DP), parameter :: graddelta = 1e-4_DP !! Delta x for gradient calculations real(DP), dimension(N) :: S !! Direction vectors real(DP), dimension(N,N) :: H !! Approximated inverse Hessian matrix @@ -56,17 +57,23 @@ module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) return end if grad1(:) = grad0(:) - do i = 1, MAXLOOP + do i = 1, maxloop !check for convergence conv = count(abs(grad1(:)) > eps) + ! write(*,*) 'loop: ', i + ! write(*,*) 'conv: ', conv + ! write(*,*) 'grad1 / eps' + ! do j = 1, N + ! write(*,*) j, abs(grad1(j)) / eps + ! end do if (conv == 0) then - !write(*,*) "BFGS converged on gradient after ",i," iterations" + ! write(*,*) "BFGS converged on gradient after ",i," iterations" exit end if S(:) = -matmul(H(:,:), grad1(:)) astar = minimize1D(f, x1, S, N, graddelta, lerr) if (lerr) then - !write(*,*) "Exiting BFGS with error in minimize1D step" + ! write(*,*) "Exiting BFGS with error in minimize1D step" exit end if ! Get new x values @@ -86,7 +93,7 @@ module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) end do ! prevent divide by zero (convergence) if (abs(Py) < tiny(Py)) then - !write(*,*) "BFGS Converged on tiny Py after ",i," iterations" + ! write(*,*) "BFGS Converged on tiny Py after ",i," iterations" exit end if ! set up update @@ -108,15 +115,15 @@ module function util_minimize_bfgs(f, N, x0, eps, lerr) result(x1) ! Stop everything if there are any exceptions to allow the routine to fail gracefully call ieee_get_flag(ieee_usual, fpe_flag) if (any(fpe_flag)) exit - if (i == MAXLOOP) then + if (i == maxloop) then lerr = .true. - !write(*,*) "BFGS ran out of loops!" + ! write(*,*) "BFGS ran out of loops!" end if end do call ieee_get_flag(ieee_usual, fpe_flag) lerr = lerr .or. any(fpe_flag) - !if (any(fpe_flag)) write(*,*) 'BFGS did not converge due to fpe' - !if (lerr) write(*,*) "BFGS did not converge!" + ! if (any(fpe_flag)) write(*,*) 'BFGS did not converge due to fpe' + ! if (lerr) write(*,*) "BFGS did not converge!" call ieee_set_status(original_fpe_status) return @@ -180,6 +187,7 @@ function gradf(f, N, x1, dx, lerr) result(grad) return end function gradf + function minimize1D(f, x0, S, N, eps, lerr) result(astar) !! - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - !! This program find the minimum of a function of N variables in a single direction @@ -253,6 +261,7 @@ function minimize1D(f, x0, S, N, eps, lerr) result(astar) return end function minimize1D + function n2one(f, x0, S, N, a, lerr) result(fnew) implicit none ! Arguments diff --git a/src/util/util_rescale.f90 b/src/util/util_rescale.f90 index 62a9409ec..50ebc088c 100644 --- a/src/util/util_rescale.f90 +++ b/src/util/util_rescale.f90 @@ -20,9 +20,11 @@ module subroutine util_rescale_system(self, param, mscale, dscale, tscale) ! Calculate the G for the system units param%GU = GC / (param%DU2M**3 / (param%MU2KG * param%TU2S**2)) - ! Calculate the inverse speed of light in the system units - param%inv_c2 = einsteinC * param%TU2S / param%DU2M - param%inv_c2 = (param%inv_c2)**(-2) + if (param%lgr) then + ! Calculate the inverse speed of light in the system units + param%inv_c2 = einsteinC * param%TU2S / param%DU2M + param%inv_c2 = (param%inv_c2)**(-2) + end if vscale = dscale / tscale diff --git a/src/util/util_resize.f90 b/src/util/util_resize.f90 index 80d87209c..dfef8771b 100644 --- a/src/util/util_resize.f90 +++ b/src/util/util_resize.f90 @@ -5,7 +5,7 @@ module subroutine util_resize_arr_char_string(arr, nnew) !! author: David A. Minton !! - !! Resizes an array component of type character string. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + !! Resizes an array component of type character string. nnew = 0 will deallocate. implicit none ! Arguments character(len=STRMAX), dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -14,21 +14,31 @@ module subroutine util_resize_arr_char_string(arr, nnew) character(len=STRMAX), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr) - if (nnew == nold) return + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if + + if (nnew == nold) return + allocate(tmp(nnew)) - if (nnew > nold) then - tmp(1:nold) = arr(1:nold) + if (nold > 0) then + if (nnew > nold) then + tmp(1:nold) = arr(1:nold) + tmp(nold+1:nnew) = "" + else + tmp(1:nnew) = arr(1:nnew) + end if else - tmp(1:nnew) = arr(1:nnew) + tmp(1:nnew) = "" end if call move_alloc(tmp, arr) @@ -39,7 +49,7 @@ end subroutine util_resize_arr_char_string module subroutine util_resize_arr_DP(arr, nnew) !! author: David A. Minton !! - !! Resizes an array component of double precision type. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + !! Resizes an array component of double precision type. Passing nnew = 0 will deallocate. implicit none ! Arguments real(DP), dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -47,22 +57,33 @@ module subroutine util_resize_arr_DP(arr, nnew) ! Internals real(DP), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size + real(DP), parameter :: init_val = 0.0_DP - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr) - if (nnew == nold) return + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if + + if (nnew == nold) return + allocate(tmp(nnew)) - if (nnew > nold) then - tmp(1:nold) = arr(1:nold) + if (nold > 0) then + if (nnew > nold) then + tmp(1:nold) = arr(1:nold) + tmp(nold+1:nnew) = init_val + else + tmp(1:nnew) = arr(1:nnew) + end if else - tmp(1:nnew) = arr(1:nnew) + tmp(1:nnew) = init_val end if call move_alloc(tmp, arr) @@ -73,7 +94,7 @@ end subroutine util_resize_arr_DP module subroutine util_resize_arr_DPvec(arr, nnew) !! author: David A. Minton !! - !! Resizes an array component of double precision vectors of size (NDIM, n). Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + !! Resizes an array component of double precision vectors of size (NDIM, n). Passing nnew = 0 will deallocate. implicit none ! Arguments real(DP), dimension(:,:), allocatable, intent(inout) :: arr !! Array to resize @@ -81,33 +102,51 @@ module subroutine util_resize_arr_DPvec(arr, nnew) ! Internals real(DP), dimension(:,:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size + real(DP), dimension(NDIM), parameter :: init_val = 0.0_DP + integer(I4B) :: i - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr, dim=2) - if (nnew == nold) return + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr, dim=2) + else + nold = 0 + end if + + if (nnew == nold) return + allocate(tmp(NDIM, nnew)) - if (nnew > nold) then - tmp(:, 1:nold) = arr(:, 1:nold) + if (nold > 0) then + if (nnew > nold) then + tmp(:,1:nold) = arr(:,1:nold) + do i = nold+1, nnew + tmp(:,i) = init_val(:) + end do + else + tmp(:,1:nnew) = arr(:,1:nnew) + end if else - tmp(:, 1:nnew) = arr(:, 1:nnew) + do i = 1, nnew + tmp(:, i) = init_val(:) + end do end if call move_alloc(tmp, arr) return + + return end subroutine util_resize_arr_DPvec module subroutine util_resize_arr_I4B(arr, nnew) !! author: David A. Minton !! - !! Resizes an array component of integer type. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + !! Resizes an array component of integer type. Passing nnew = 0 will deallocate. implicit none ! Arguments integer(I4B), dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -115,33 +154,84 @@ module subroutine util_resize_arr_I4B(arr, nnew) ! Internals integer(I4B), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size + integer(I4B), parameter :: init_val = -1 + + if (nnew < 0) return - if (.not. allocated(arr) .or. nnew < 0) return + if (nnew == 0) then + if (allocated(arr)) deallocate(arr) + return + end if + + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if - nold = size(arr) if (nnew == nold) return + + allocate(tmp(nnew)) + if (nold > 0) then + if (nnew > nold) then + tmp(1:nold) = arr(1:nold) + tmp(nold+1:nnew) = init_val + else + tmp(1:nnew) = arr(1:nnew) + end if + else + tmp(1:nnew) = init_val + end if + call move_alloc(tmp, arr) + + return + end subroutine util_resize_arr_I4B + + + module subroutine util_resize_arr_info(arr, nnew) + !! author: David A. Minton + !! + !! Resizes an array component of type character string. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + implicit none + ! Arguments + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Array to resize + integer(I4B), intent(in) :: nnew !! New size + ! Internals + type(swiftest_particle_info), dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated + integer(I4B) :: nold !! Old size + + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if + + if (nnew == nold) return + allocate(tmp(nnew)) if (nnew > nold) then - tmp(1:nold) = arr(1:nold) + call util_copy_particle_info_arr(arr(1:nold), tmp(1:nold)) else - tmp(1:nnew) = arr(1:nnew) + call util_copy_particle_info_arr(arr(1:nnew), tmp(1:nnew)) end if + call move_alloc(tmp, arr) return - end subroutine util_resize_arr_I4B + end subroutine util_resize_arr_info module subroutine util_resize_arr_logical(arr, nnew) !! author: David A. Minton !! - !! Resizes an array component of logical type. Array will only be resized if has previously been allocated. Passing nnew = 0 will deallocate. + !! Resizes an array component of logical type. Passing nnew = 0 will deallocate. implicit none ! Arguments logical, dimension(:), allocatable, intent(inout) :: arr !! Array to resize @@ -149,22 +239,33 @@ module subroutine util_resize_arr_logical(arr, nnew) ! Internals logical, dimension(:), allocatable :: tmp !! Temporary storage array in case the input array is already allocated integer(I4B) :: nold !! Old size + logical, parameter :: init_val = .false. - if (.not. allocated(arr) .or. nnew < 0) return - - nold = size(arr) - if (nnew == nold) return + if (nnew < 0) return if (nnew == 0) then - deallocate(arr) + if (allocated(arr)) deallocate(arr) return end if + if (allocated(arr)) then + nold = size(arr) + else + nold = 0 + end if + + if (nnew == nold) return + allocate(tmp(nnew)) - if (nnew > nold) then - tmp(1:nold) = arr(1:nold) + if (nold > 0) then + if (nnew > nold) then + tmp(1:nold) = arr(1:nold) + tmp(nold+1:nnew) = init_val + else + tmp(1:nnew) = arr(1:nnew) + end if else - tmp(1:nnew) = arr(1:nnew) + tmp(1:nnew) = init_val end if call move_alloc(tmp, arr) @@ -178,10 +279,10 @@ module subroutine util_resize_body(self, nnew) !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. implicit none ! Arguments - class(swiftest_body), intent(inout) :: self !! Swiftest body object - integer(I4B), intent(in) :: nnew !! New size neded + class(swiftest_body), intent(inout) :: self !! Swiftest body object + integer(I4B), intent(in) :: nnew !! New size neded - call util_resize(self%name, nnew) + call util_resize(self%info, nnew) call util_resize(self%id, nnew) call util_resize(self%status, nnew) call util_resize(self%ldiscard, nnew) @@ -249,7 +350,7 @@ end subroutine util_resize_encounter module subroutine util_resize_pl(self, nnew) !! author: David A. Minton !! - !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. + !! Checks the current size of a Swiftest massive body against the requested size and resizes it if it is too small. implicit none ! Arguments class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object @@ -270,7 +371,8 @@ module subroutine util_resize_pl(self, nnew) call util_resize(self%k2, nnew) call util_resize(self%Q, nnew) call util_resize(self%tlag, nnew) - call self%eucl_index() + + if (allocated(self%k_plpl)) deallocate(self%k_plpl) return end subroutine util_resize_pl @@ -279,10 +381,10 @@ end subroutine util_resize_pl module subroutine util_resize_tp(self, nnew) !! author: David A. Minton !! - !! Checks the current size of a Swiftest body against the requested size and resizes it if it is too small. + !! Checks the current size of a Swiftest test particle against the requested size and resizes it if it is too small. implicit none ! Arguments - class(swiftest_tp), intent(inout) :: self !! Swiftest massive body object + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object integer(I4B), intent(in) :: nnew !! New size neded call util_resize_body(self, nnew) diff --git a/src/util/util_set.f90 b/src/util/util_set.f90 index 86e021ab6..80ed89b1f 100644 --- a/src/util/util_set.f90 +++ b/src/util/util_set.f90 @@ -77,7 +77,7 @@ module subroutine util_set_mu_pl(self, cb) class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - if (self%nbody > 0) self%mu(:) = cb%Gmass + self%Gmass(:) + if (self%nbody > 0) self%mu(1:self%nbody) = cb%Gmass + self%Gmass(1:self%nbody) return end subroutine util_set_mu_pl @@ -92,11 +92,74 @@ module subroutine util_set_mu_tp(self, cb) class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - if (self%nbody > 0) self%mu(:) = cb%Gmass + if (self%nbody == 0) return + self%mu(1:self%nbody) = cb%Gmass return end subroutine util_set_mu_tp + module subroutine util_set_particle_info(self, name, particle_type, status, origin_type, origin_time, origin_xh, origin_vh, discard_time, discard_xh, discard_vh, discard_body_id) + !! author: David A. Minton + !! + !! Sets one or more values of the particle information metadata object + implicit none + ! Arguments + class(swiftest_particle_info), intent(inout) :: self + character(len=*), intent(in), optional :: name !! Non-unique name + character(len=*), intent(in), optional :: particle_type !! String containing a description of the particle type (e.g. Central Body, Massive Body, Test Particle) + character(len=*), intent(in), optional :: status !! Particle status description: ACTIVE, MERGED, FRAGMENTED, etc. + character(len=*), intent(in), optional :: origin_type !! String containing a description of the origin of the particle (e.g. Initial Conditions, Supercatastrophic, Disruption, etc.) + real(DP), intent(in), optional :: origin_time !! The time of the particle's formation + real(DP), dimension(:), intent(in), optional :: origin_xh !! The heliocentric distance vector at the time of the particle's formation + real(DP), dimension(:), intent(in), optional :: origin_vh !! The heliocentric velocity vector at the time of the particle's formation + real(DP), intent(in), optional :: discard_time !! The time of the particle's discard + real(DP), dimension(:), intent(in), optional :: discard_xh !! The heliocentric distance vector at the time of the particle's discard + real(DP), dimension(:), intent(in), optional :: discard_vh !! The heliocentric velocity vector at the time of the particle's discard + integer(I4B), intent(in), optional :: discard_body_id !! The id of the other body involved in the discard (0 if no other body involved) + ! Internals + character(len=NAMELEN) :: lenstr + character(len=:), allocatable :: fmtlabel + + write(lenstr, *) NAMELEN + fmtlabel = "(A" // trim(adjustl(lenstr)) // ")" + + if (present(name)) then + write(self%name, fmtlabel) trim(adjustl(name)) + end if + if (present(particle_type)) then + write(self%particle_type, fmtlabel) trim(adjustl(particle_type)) + end if + if (present(status)) then + write(self%status, fmtlabel) trim(adjustl(status)) + end if + if (present(origin_type)) then + write(self%origin_type, fmtlabel) trim(adjustl(origin_type)) + end if + if (present(origin_time)) then + self%origin_time = origin_time + end if + if (present(origin_xh)) then + self%origin_xh(:) = origin_xh(:) + end if + if (present(origin_vh)) then + self%origin_vh(:) = origin_vh(:) + end if + if (present(discard_time)) then + self%discard_time = discard_time + end if + if (present(discard_xh)) then + self%discard_xh(:) = discard_xh(:) + end if + if (present(discard_vh)) then + self%discard_vh(:) = discard_vh(:) + end if + if (present(discard_body_id)) then + self%discard_body_id = discard_body_id + end if + + return + end subroutine util_set_particle_info + module subroutine util_set_rhill(self,cb) !! author: David A. Minton @@ -107,10 +170,10 @@ module subroutine util_set_rhill(self,cb) class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object class(swiftest_cb), intent(inout) :: cb !! Swiftest central body object - if (self%nbody > 0) then - call self%xv2el(cb) - self%rhill(:) = self%a(:) * (self%Gmass(:) / cb%Gmass / 3)**THIRD - end if + if (self%nbody == 0) return + + call self%xv2el(cb) + self%rhill(1:self%nbody) = self%a(1:self%nbody) * (self%Gmass(1:self%nbody) / cb%Gmass / 3)**THIRD return end subroutine util_set_rhill @@ -127,10 +190,10 @@ module subroutine util_set_rhill_approximate(self,cb) ! Internals real(DP), dimension(:), allocatable :: rh - if (self%nbody > 0) then - rh(:) = .mag. self%xh(:,:) - self%rhill(:) = rh(:) * (self%Gmass(:) / cb%Gmass / 3)**THIRD - end if + if (self%nbody == 0) return + + rh(1:self%nbody) = .mag. self%xh(:,1:self%nbody) + self%rhill(1:self%nbody) = rh(1:self%nbody) * (self%Gmass(1:self%nbody) / cb%Gmass / 3)**THIRD return end subroutine util_set_rhill_approximate diff --git a/src/util/util_sort.f90 b/src/util/util_sort.f90 index 752e78ab7..b69627b0b 100644 --- a/src/util/util_sort.f90 +++ b/src/util/util_sort.f90 @@ -13,9 +13,11 @@ module subroutine util_sort_body(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction + if (self%nbody == 0) return + if (ascending) then direction = 1 else @@ -23,6 +25,7 @@ module subroutine util_sort_body(self, sortby, ascending) end if associate(body => self, n => self%nbody) + allocate(ind(n)) select case(sortby) case("id") call util_sort(direction * body%id(1:n), ind(1:n)) @@ -55,6 +58,174 @@ module subroutine util_sort_body(self, sortby, ascending) end subroutine util_sort_body + module subroutine util_sort_dp(arr) + !! author: David A. Minton + !! + !! Sort input double precision array in place into ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + !! + implicit none + ! Arguments + real(DP), dimension(:), intent(inout) :: arr + ! Internals + real(DP) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + do i = 2, n + tmp = arr(i) + do j = i - 1, 1, -1 + if (arr(j) <= tmp) exit + arr(j + 1) = arr(j) + end do + arr(j + 1) = tmp + end do + + return + end subroutine util_sort_dp + + + module subroutine util_sort_index_dp(arr, ind) + !! author: David A. Minton + !! + !! Sort input double precision array by index in ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + !! + implicit none + ! Arguments + real(DP), dimension(:), intent(in) :: arr + integer(I4B), dimension(:), intent(out) :: ind + ! Internals + real(DP) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + ind = [(i, i=1, n)] + do i = 2, n + tmp = arr(ind(i)) + do j = i - 1, 1, -1 + if (arr(ind(j)) <= tmp) exit + ind(j + 1) = ind(j) + end do + ind(j + 1) = i + end do + + return + end subroutine util_sort_index_dp + + + module subroutine util_sort_i4b(arr) + !! author: David A. Minton + !! + !! Sort input integer array in place into ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + !! + implicit none + ! Arguments + integer(I4B), dimension(:), intent(inout) :: arr + ! Internals + integer(I4B) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + do i = 2, n + tmp = arr(i) + do j = i - 1, 1, -1 + if (arr(j) <= tmp) exit + arr(j + 1) = arr(j) + end do + arr(j + 1) = tmp + end do + + return + end subroutine util_sort_i4b + + + module subroutine util_sort_index_i4b(arr, ind) + !! author: David A. Minton + !! + !! Sort input integer array by index in ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + !! + implicit none + ! Arguments + integer(I4B), dimension(:), intent(in) :: arr + integer(I4B), dimension(:), intent(out) :: ind + ! Internals + integer(I4B) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + ind = [(i, i=1, n)] + do i = 2, n + tmp = arr(ind(i)) + do j = i - 1, 1, -1 + if (arr(ind(j)) <= tmp) exit + ind(j + 1) = ind(j) + end do + ind(j + 1) = i + end do + + return + end subroutine util_sort_index_i4b + + + module subroutine util_sort_sp(arr) + !! author: David A. Minton + !! + !! Sort input single precision array in place into ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + ! + implicit none + ! Arguments + real(SP), dimension(:), intent(inout) :: arr + ! Internals + real(SP) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + do i = 2, n + tmp = arr(i) + do j = i - 1, 1, -1 + if (arr(j) <= tmp) exit + arr(j + 1) = arr(j) + end do + arr(j + 1) = tmp + end do + + return + end subroutine util_sort_sp + + + module subroutine util_sort_index_sp(arr, ind) + !! author: David A. Minton + !! + !! Sort input single precision array by index in ascending numerical order using insertion sort. + !! This algorithm works well for partially sorted arrays (which is usually the case here) + !! + implicit none + ! Arguments + real(SP), dimension(:), intent(in) :: arr + integer(I4B), dimension(:), intent(out) :: ind + ! Internals + real(SP) :: tmp + integer(I4B) :: n, i, j + + n = size(arr) + ind = [(i, i=1, n)] + do i = 2, n + tmp = arr(ind(i)) + do j = i - 1, 1, -1 + if (arr(ind(j)) <= tmp) exit + ind(j + 1) = ind(j) + end do + ind(j + 1) = i + end do + + return + end subroutine util_sort_index_sp + + module subroutine util_sort_pl(self, sortby, ascending) !! author: David A. Minton !! @@ -66,9 +237,11 @@ module subroutine util_sort_pl(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction + if (self%nbody == 0) return + if (ascending) then direction = 1 else @@ -76,6 +249,7 @@ module subroutine util_sort_pl(self, sortby, ascending) end if associate(pl => self, npl => self%nbody) + allocate(ind(npl)) select case(sortby) case("Gmass","mass") call util_sort(direction * pl%Gmass(1:npl), ind(1:npl)) @@ -117,9 +291,11 @@ module subroutine util_sort_tp(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction + if (self%nbody == 0) return + if (ascending) then direction = 1 else @@ -127,6 +303,7 @@ module subroutine util_sort_tp(self, sortby, ascending) end if associate(tp => self, ntp => self%nbody) + allocate(ind(ntp)) select case(sortby) case("peri") call util_sort(direction * tp%peri(1:ntp), ind(1:ntp)) @@ -156,264 +333,215 @@ module subroutine util_sort_rearrange_body(self, ind) ! Arguments class(swiftest_body), intent(inout) :: self !! Swiftest body object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - ! Internals - class(swiftest_body), allocatable :: body_sorted !! Temporary holder for sorted body associate(n => self%nbody) - allocate(body_sorted, source=self) - if (allocated(self%id)) self%id(1:n) = body_sorted%id(ind(1:n)) - if (allocated(self%name)) self%name(1:n) = body_sorted%name(ind(1:n)) - if (allocated(self%status)) self%status(1:n) = body_sorted%status(ind(1:n)) - if (allocated(self%ldiscard)) self%ldiscard(1:n) = body_sorted%ldiscard(ind(1:n)) - if (allocated(self%xh)) self%xh(:,1:n) = body_sorted%xh(:,ind(1:n)) - if (allocated(self%vh)) self%vh(:,1:n) = body_sorted%vh(:,ind(1:n)) - if (allocated(self%xb)) self%xb(:,1:n) = body_sorted%xb(:,ind(1:n)) - if (allocated(self%vb)) self%vb(:,1:n) = body_sorted%vb(:,ind(1:n)) - if (allocated(self%ah)) self%ah(:,1:n) = body_sorted%ah(:,ind(1:n)) - if (allocated(self%ir3h)) self%ir3h(1:n) = body_sorted%ir3h(ind(1:n)) - if (allocated(self%mu)) self%mu(1:n) = body_sorted%mu(ind(1:n)) - if (allocated(self%lmask)) self%lmask(1:n) = body_sorted%lmask(ind(1:n)) - if (allocated(self%a)) self%a(1:n) = body_sorted%a(ind(1:n)) - if (allocated(self%e)) self%e(1:n) = body_sorted%e(ind(1:n)) - if (allocated(self%inc)) self%inc(1:n) = body_sorted%inc(ind(1:n)) - if (allocated(self%capom)) self%capom(1:n) = body_sorted%capom(ind(1:n)) - if (allocated(self%omega)) self%omega(1:n) = body_sorted%omega(ind(1:n)) - if (allocated(self%capm)) self%capm(1:n) = body_sorted%capm(ind(1:n)) - if (allocated(self%aobl)) self%aobl(:,1:n) = body_sorted%aobl(:,ind(1:n)) - if (allocated(self%atide)) self%atide(:,1:n) = body_sorted%atide(:,ind(1:n)) - if (allocated(self%agr)) self%agr(:,1:n) = body_sorted%agr(:,ind(1:n)) - deallocate(body_sorted) + call util_sort_rearrange(self%id, ind, n) + call util_sort_rearrange(self%info, ind, n) + call util_sort_rearrange(self%status, ind, n) + call util_sort_rearrange(self%ldiscard, ind, n) + call util_sort_rearrange(self%xh, ind, n) + call util_sort_rearrange(self%vh, ind, n) + call util_sort_rearrange(self%xb, ind, n) + call util_sort_rearrange(self%vb, ind, n) + call util_sort_rearrange(self%ah, ind, n) + call util_sort_rearrange(self%ir3h, ind, n) + call util_sort_rearrange(self%mu, ind, n) + call util_sort_rearrange(self%lmask, ind, n) + call util_sort_rearrange(self%a, ind, n) + call util_sort_rearrange(self%e, ind, n) + call util_sort_rearrange(self%inc, ind, n) + call util_sort_rearrange(self%capom, ind, n) + call util_sort_rearrange(self%omega, ind, n) + call util_sort_rearrange(self%capm, ind, n) + call util_sort_rearrange(self%aobl, ind, n) + call util_sort_rearrange(self%atide, ind, n) + call util_sort_rearrange(self%agr, ind, n) end associate return end subroutine util_sort_rearrange_body - module subroutine util_sort_rearrange_pl(self, ind) + module subroutine util_sort_rearrange_arr_char_string(arr, ind, n) !! author: David A. Minton !! - !! Rearrange Swiftest massive body structure in-place from an index list. - !! This is a helper utility used to make polymorphic sorting work on Swiftest structures. + !! Rearrange a single array of character string in-place from an index list. implicit none - class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object - integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) + ! Arguments + character(len=STRMAX), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - class(swiftest_pl), allocatable :: pl_sorted !! Temporary holder for sorted body + character(len=STRMAX), dimension(:), allocatable :: tmp !! Temporary copy of arry used during rearrange operation - associate(pl => self, npl => self%nbody) - call util_sort_rearrange_body(pl,ind) - allocate(pl_sorted, source=self) - if (allocated(pl%mass)) pl%mass(1:npl) = pl_sorted%mass(ind(1:npl)) - if (allocated(pl%Gmass)) pl%Gmass(1:npl) = pl_sorted%Gmass(ind(1:npl)) - if (allocated(pl%rhill)) pl%rhill(1:npl) = pl_sorted%rhill(ind(1:npl)) - if (allocated(pl%xbeg)) pl%xbeg(:,1:npl) = pl_sorted%xbeg(:,ind(1:npl)) - if (allocated(pl%xend)) pl%xend(:,1:npl) = pl_sorted%xend(:,ind(1:npl)) - if (allocated(pl%vbeg)) pl%vbeg(:,1:npl) = pl_sorted%vbeg(:,ind(1:npl)) - if (allocated(pl%radius)) pl%radius(1:npl) = pl_sorted%radius(ind(1:npl)) - if (allocated(pl%density)) pl%density(1:npl) = pl_sorted%density(ind(1:npl)) - if (allocated(pl%Ip)) pl%Ip(:,1:npl) = pl_sorted%Ip(:,ind(1:npl)) - if (allocated(pl%rot)) pl%rot(:,1:npl) = pl_sorted%rot(:,ind(1:npl)) - if (allocated(pl%k2)) pl%k2(1:npl) = pl_sorted%k2(ind(1:npl)) - if (allocated(pl%Q)) pl%Q(1:npl) = pl_sorted%Q(ind(1:npl)) - if (allocated(pl%tlag)) pl%tlag(1:npl) = pl_sorted%tlag(ind(1:npl)) - - deallocate(pl_sorted) - end associate + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + tmp(1:n) = arr(ind(1:n)) + call move_alloc(tmp, arr) return - end subroutine util_sort_rearrange_pl + end subroutine util_sort_rearrange_arr_char_string - module subroutine util_sort_rearrange_tp(self, ind) + module subroutine util_sort_rearrange_arr_DP(arr, ind, n) !! author: David A. Minton !! - !! Rearrange Swiftest massive body structure in-place from an index list. - !! This is a helper utility used to make polymorphic sorting work on Swiftest structures. + !! Rearrange a single array of DP type in-place from an index list. implicit none ! Arguments - class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object - integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) + real(DP), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - class(swiftest_tp), allocatable :: tp_sorted !! Temporary holder for sorted body + real(DP), dimension(:), allocatable :: tmp !! Temporary copy of array used during rearrange operation - associate(tp => self, ntp => self%nbody) - call util_sort_rearrange_body(tp,ind) - allocate(tp_sorted, source=self) - if (allocated(tp%isperi)) tp%isperi(1:ntp) = tp_sorted%isperi(ind(1:ntp)) - if (allocated(tp%peri)) tp%peri(1:ntp) = tp_sorted%peri(ind(1:ntp)) - if (allocated(tp%atp)) tp%atp(1:ntp) = tp_sorted%atp(ind(1:ntp)) - deallocate(tp_sorted) - end associate + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + tmp(1:n) = arr(ind(1:n)) + call move_alloc(tmp, arr) return - end subroutine util_sort_rearrange_tp + end subroutine util_sort_rearrange_arr_DP - module subroutine util_sort_dp(arr) + module subroutine util_sort_rearrange_arr_DPvec(arr, ind, n) !! author: David A. Minton !! - !! Sort input double precision array in place into ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - !! + !! Rearrange a single array of (NDIM,n) DP-type vectors in-place from an index list. implicit none ! Arguments - real(DP), dimension(:), intent(inout) :: arr + real(DP), dimension(:,:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - real(DP) :: tmp - integer(I4B) :: n, i, j + real(DP), dimension(:,:), allocatable :: tmp !! Temporary copy of array used during rearrange operation - n = size(arr) - do i = 2, n - tmp = arr(i) - do j = i - 1, 1, -1 - if (arr(j) <= tmp) exit - arr(j + 1) = arr(j) - end do - arr(j + 1) = tmp - end do + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + tmp(:,1:n) = arr(:, ind(1:n)) + call move_alloc(tmp, arr) return - end subroutine util_sort_dp + end subroutine util_sort_rearrange_arr_DPvec - module subroutine util_sort_index_dp(arr, ind) + module subroutine util_sort_rearrange_arr_I4B(arr, ind, n) !! author: David A. Minton !! - !! Sort input double precision array by index in ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - !! + !! Rearrange a single array of integers in-place from an index list. implicit none ! Arguments - real(DP), dimension(:), intent(in) :: arr - integer(I4B), dimension(:), intent(out) :: ind + integer(I4B), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - real(DP) :: tmp - integer(I4B) :: n, i, j + integer(I4B), dimension(:), allocatable :: tmp !! Temporary copy of array used during rearrange operation - n = size(arr) - ind = [(i, i=1, n)] - do i = 2, n - tmp = arr(ind(i)) - do j = i - 1, 1, -1 - if (arr(ind(j)) <= tmp) exit - ind(j + 1) = ind(j) - end do - ind(j + 1) = i - end do + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + tmp(1:n) = arr(ind(1:n)) + call move_alloc(tmp, arr) return - end subroutine util_sort_index_dp + end subroutine util_sort_rearrange_arr_I4B - module subroutine util_sort_i4b(arr) + module subroutine util_sort_rearrange_arr_logical(arr, ind, n) !! author: David A. Minton !! - !! Sort input integer array in place into ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - !! + !! Rearrange a single array of logicals in-place from an index list. implicit none ! Arguments - integer(I4B), dimension(:), intent(inout) :: arr + logical, dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - integer(I4B) :: tmp - integer(I4B) :: n, i, j + logical, dimension(:), allocatable :: tmp !! Temporary copy of array used during rearrange operation - n = size(arr) - do i = 2, n - tmp = arr(i) - do j = i - 1, 1, -1 - if (arr(j) <= tmp) exit - arr(j + 1) = arr(j) - end do - arr(j + 1) = tmp - end do + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + tmp(1:n) = arr(ind(1:n)) + call move_alloc(tmp, arr) return - end subroutine util_sort_i4b + end subroutine util_sort_rearrange_arr_logical - module subroutine util_sort_index_i4b(arr, ind) + module subroutine util_sort_rearrange_arr_info(arr, ind, n) !! author: David A. Minton !! - !! Sort input integer array by index in ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - !! + !! Rearrange a single array of particle information type in-place from an index list. implicit none ! Arguments - integer(I4B), dimension(:), intent(in) :: arr - integer(I4B), dimension(:), intent(out) :: ind + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: arr !! Destination array + integer(I4B), dimension(:), intent(in) :: ind !! Index to rearrange against + integer(I4B), intent(in) :: n !! Number of elements in arr and ind to rearrange ! Internals - integer(I4B) :: tmp - integer(I4B) :: n, i, j + type(swiftest_particle_info), dimension(:), allocatable :: tmp !! Temporary copy of array used during rearrange operation + integer(I4B) :: i - n = size(arr) - ind = [(i, i=1, n)] - do i = 2, n - tmp = arr(ind(i)) - do j = i - 1, 1, -1 - if (arr(ind(j)) <= tmp) exit - ind(j + 1) = ind(j) - end do - ind(j + 1) = i - end do + + if (.not. allocated(arr) .or. n <= 0) return + allocate(tmp, mold=arr) + + call util_copy_particle_info_arr(arr, tmp, ind) + call move_alloc(tmp, arr) return - end subroutine util_sort_index_i4b + end subroutine util_sort_rearrange_arr_info - module subroutine util_sort_sp(arr) + module subroutine util_sort_rearrange_pl(self, ind) !! author: David A. Minton !! - !! Sort input single precision array in place into ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - ! + !! Rearrange Swiftest massive body structure in-place from an index list. + !! This is a helper utility used to make polymorphic sorting work on Swiftest structures. implicit none - ! Arguments - real(SP), dimension(:), intent(inout) :: arr - ! Internals - real(SP) :: tmp - integer(I4B) :: n, i, j + class(swiftest_pl), intent(inout) :: self !! Swiftest massive body object + integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - n = size(arr) - do i = 2, n - tmp = arr(i) - do j = i - 1, 1, -1 - if (arr(j) <= tmp) exit - arr(j + 1) = arr(j) - end do - arr(j + 1) = tmp - end do + associate(pl => self, npl => self%nbody) + call util_sort_rearrange(pl%mass, ind, npl) + call util_sort_rearrange(pl%Gmass, ind, npl) + call util_sort_rearrange(pl%rhill, ind, npl) + call util_sort_rearrange(pl%xbeg, ind, npl) + call util_sort_rearrange(pl%vbeg, ind, npl) + call util_sort_rearrange(pl%radius, ind, npl) + call util_sort_rearrange(pl%density, ind, npl) + call util_sort_rearrange(pl%Ip, ind, npl) + call util_sort_rearrange(pl%rot, ind, npl) + call util_sort_rearrange(pl%k2, ind, npl) + call util_sort_rearrange(pl%Q, ind, npl) + call util_sort_rearrange(pl%tlag, ind, npl) + + if (allocated(pl%k_plpl)) deallocate(pl%k_plpl) + + call util_sort_rearrange_body(pl, ind) + end associate return - end subroutine util_sort_sp + end subroutine util_sort_rearrange_pl - module subroutine util_sort_index_sp(arr, ind) + module subroutine util_sort_rearrange_tp(self, ind) !! author: David A. Minton !! - !! Sort input single precision array by index in ascending numerical order using insertion sort. - !! This algorithm works well for partially sorted arrays (which is usually the case here) - !! + !! Rearrange Swiftest massive body structure in-place from an index list. + !! This is a helper utility used to make polymorphic sorting work on Swiftest structures. implicit none ! Arguments - real(SP), dimension(:), intent(in) :: arr - integer(I4B), dimension(:), intent(out) :: ind - ! Internals - real(SP) :: tmp - integer(I4B) :: n, i, j + class(swiftest_tp), intent(inout) :: self !! Swiftest test particle object + integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - n = size(arr) - ind = [(i, i=1, n)] - do i = 2, n - tmp = arr(ind(i)) - do j = i - 1, 1, -1 - if (arr(ind(j)) <= tmp) exit - ind(j + 1) = ind(j) - end do - ind(j + 1) = i - end do + associate(tp => self, ntp => self%nbody) + call util_sort_rearrange(tp%isperi, ind, ntp) + call util_sort_rearrange(tp%peri, ind, ntp) + call util_sort_rearrange(tp%atp, ind, ntp) + + call util_sort_rearrange_body(tp, ind) + end associate return - end subroutine util_sort_index_sp + end subroutine util_sort_rearrange_tp end submodule s_util_sort diff --git a/src/util/util_spill.f90 b/src/util/util_spill.f90 index 9c76ff5e9..16039c4da 100644 --- a/src/util/util_spill.f90 +++ b/src/util/util_spill.f90 @@ -13,14 +13,28 @@ module subroutine util_spill_arr_char_string(keeps, discards, lspill_list, ldest character(len=STRMAX), dimension(:), allocatable, intent(inout) :: discards !! Array of discards logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: nspill, nkeep, nlist + character(len=STRMAX), dimension(:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) + if (nkeep > 0) then + allocate(tmp(nkeep)) + tmp(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) + call move_alloc(tmp, keeps) else deallocate(keeps) end if @@ -28,6 +42,7 @@ module subroutine util_spill_arr_char_string(keeps, discards, lspill_list, ldest return end subroutine util_spill_arr_char_string + module subroutine util_spill_arr_DP(keeps, discards, lspill_list, ldestructive) !! author: David A. Minton @@ -40,14 +55,28 @@ module subroutine util_spill_arr_DP(keeps, discards, lspill_list, ldestructive) real(DP), dimension(:), allocatable, intent(inout) :: discards !! Array of discards logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: nspill, nkeep, nlist + real(DP), dimension(:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) + if (nkeep > 0) then + allocate(tmp(nkeep)) + tmp(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) + call move_alloc(tmp, keeps) else deallocate(keeps) end if @@ -56,6 +85,7 @@ module subroutine util_spill_arr_DP(keeps, discards, lspill_list, ldestructive) return end subroutine util_spill_arr_DP + module subroutine util_spill_arr_DPvec(keeps, discards, lspill_list, ldestructive) !! author: David A. Minton !! @@ -68,25 +98,40 @@ module subroutine util_spill_arr_DPvec(keeps, discards, lspill_list, ldestructiv logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not ! Internals - integer(I4B) :: i - - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(NDIM, count(lspill_list(:)))) + integer(I4B) :: i, nspill, nkeep, nlist + real(DP), dimension(:,:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(NDIM, nspill)) + else if (size(discards, dim=2) /= nspill) then + deallocate(discards) + allocate(discards(NDIM, nspill)) + end if do i = 1, NDIM - discards(i,:) = pack(keeps(i,:), lspill_list(:)) + discards(i,:) = pack(keeps(i,1:nlist), lspill_list(1:nlist)) end do if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then + if (nkeep > 0) then + allocate(tmp(NDIM, nkeep)) do i = 1, NDIM - keeps(i,:) = pack(keeps(i,:), .not. lspill_list(:)) + tmp(i, :) = pack(keeps(i, 1:nlist), .not. lspill_list(1:nlist)) end do + call move_alloc(tmp, keeps) + else + deallocate(keeps) end if end if return end subroutine util_spill_arr_DPvec + module subroutine util_spill_arr_I4B(keeps, discards, lspill_list, ldestructive) !! author: David A. Minton !! @@ -98,14 +143,28 @@ module subroutine util_spill_arr_I4B(keeps, discards, lspill_list, ldestructive) integer(I4B), dimension(:), allocatable, intent(inout) :: discards !! Array of discards logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: nspill, nkeep, nlist + integer(I4B), dimension(:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) + if (nkeep > 0) then + allocate(tmp(nkeep)) + tmp(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) + call move_alloc(tmp, keeps) else deallocate(keeps) end if @@ -114,6 +173,97 @@ module subroutine util_spill_arr_I4B(keeps, discards, lspill_list, ldestructive) return end subroutine util_spill_arr_I4B + + module subroutine util_spill_arr_I8B(keeps, discards, lspill_list, ldestructive) + !! author: David A. Minton + !! + !! Performs a spill operation on a single array of type I4B + !! This is the inverse of a spill operation + implicit none + ! Arguments + integer(I8B), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + integer(I8B), dimension(:), allocatable, intent(inout) :: discards !! Array of discards + logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards + logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: nspill, nkeep, nlist + integer(I8B), dimension(:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if + + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) + if (ldestructive) then + if (nkeep > 0) then + allocate(tmp(nkeep)) + tmp(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) + call move_alloc(tmp, keeps) + else + deallocate(keeps) + end if + end if + + return + end subroutine util_spill_arr_I8B + + + module subroutine util_spill_arr_info(keeps, discards, lspill_list, ldestructive) + !! author: David A. Minton + !! + !! Performs a spill operation on a single array of particle origin information types + !! This is the inverse of a spill operation + implicit none + ! Arguments + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: keeps !! Array of values to keep + type(swiftest_particle_info), dimension(:), allocatable, intent(inout) :: discards !! Array of discards + logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discardss + logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or not + ! Internals + integer(I4B) :: i, nspill, nkeep, nlist + integer(I4B), dimension(:), allocatable :: idx + type(swiftest_particle_info), dimension(:), allocatable :: tmp + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if + + allocate(idx(nspill)) + idx(:) = pack([(i, i = 1, nlist)], lspill_list) + call util_copy_particle_info_arr(keeps, discards, idx) + if (ldestructive) then + if (nkeep > 0) then + deallocate(idx) + allocate(idx(nkeep)) + allocate(tmp(nkeep)) + idx(:) = pack([(i, i = 1, nlist)], .not. lspill_list) + call util_copy_particle_info_arr(keeps, tmp, idx) + call move_alloc(tmp, keeps) + else + deallocate(keeps) + end if + end if + + return + end subroutine util_spill_arr_info + + module subroutine util_spill_arr_logical(keeps, discards, lspill_list, ldestructive) !! author: David A. Minton !! @@ -125,14 +275,28 @@ module subroutine util_spill_arr_logical(keeps, discards, lspill_list, ldestruct logical, dimension(:), allocatable, intent(inout) :: discards !! Array of discards logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter the keeps array or no + ! Internals + integer(I4B) :: nspill, nkeep, nlist + logical, dimension(:), allocatable :: tmp !! Array of values to keep + + nkeep = count(.not.lspill_list(:)) + nspill = count(lspill_list(:)) + nlist = size(lspill_list(:)) + + if (.not.allocated(keeps) .or. nspill == 0) return + if (.not.allocated(discards)) then + allocate(discards(nspill)) + else if (size(discards) /= nspill) then + deallocate(discards) + allocate(discards(nspill)) + end if - if (.not.allocated(keeps) .or. count(lspill_list(:)) == 0) return - if (.not.allocated(discards)) allocate(discards(count(lspill_list(:)))) - - discards(:) = pack(keeps(:), lspill_list(:)) + discards(:) = pack(keeps(1:nlist), lspill_list(1:nlist)) if (ldestructive) then - if (count(.not.lspill_list(:)) > 0) then - keeps(:) = pack(keeps(:), .not. lspill_list(:)) + if (nkeep > 0) then + allocate(tmp(nkeep)) + tmp(:) = pack(keeps(1:nlist), .not. lspill_list(1:nlist)) + call move_alloc(tmp, keeps) else deallocate(keeps) end if @@ -154,13 +318,14 @@ module subroutine util_spill_body(self, discards, lspill_list, ldestructive) logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list ! Internals - integer(I4B) :: i + integer(I4B) :: nbody_old ! For each component, pack the discarded bodies into the discard object and do the inverse with the keeps !> Spill all the common components associate(keeps => self) + call util_spill(keeps%id, discards%id, lspill_list, ldestructive) - call util_spill(keeps%name, discards%name, lspill_list, ldestructive) + call util_spill(keeps%info, discards%info, lspill_list, ldestructive) call util_spill(keeps%status, discards%status, lspill_list, ldestructive) call util_spill(keeps%lmask, discards%lmask, lspill_list, ldestructive) call util_spill(keeps%ldiscard, discards%ldiscard, lspill_list, ldestructive) @@ -180,17 +345,18 @@ module subroutine util_spill_body(self, discards, lspill_list, ldestructive) call util_spill(keeps%omega, discards%omega, lspill_list, ldestructive) call util_spill(keeps%capm, discards%capm, lspill_list, ldestructive) + nbody_old = keeps%nbody + ! This is the base class, so will be the last to be called in the cascade. ! Therefore we need to set the nbody values for both the keeps and discareds - discards%nbody = count(lspill_list(:)) - keeps%nbody = keeps%nbody - discards%nbody - if (keeps%nbody > size(keeps%status)) keeps%status(keeps%nbody+1:size(keeps%status)) = INACTIVE - + discards%nbody = count(lspill_list(1:nbody_old)) + if (ldestructive) keeps%nbody = nbody_old- discards%nbody end associate return end subroutine util_spill_body + module subroutine util_spill_encounter(self, discards, lspill_list, ldestructive) !! author: David A. Minton !! @@ -202,24 +368,28 @@ module subroutine util_spill_encounter(self, discards, lspill_list, ldestructive logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list ! Internals - integer(I4B) :: i + integer(I4B) :: nenc_old associate(keeps => self) - call util_spill(keeps%lvdotr, discards%lvdotr, lspill_list, ldestructive) call util_spill(keeps%status, discards%status, lspill_list, ldestructive) + call util_spill(keeps%kidx, discards%kidx, lspill_list, ldestructive) call util_spill(keeps%index1, discards%index1, lspill_list, ldestructive) call util_spill(keeps%index2, discards%index2, lspill_list, ldestructive) + call util_spill(keeps%id1, discards%id1, lspill_list, ldestructive) + call util_spill(keeps%id2, discards%id2, lspill_list, ldestructive) call util_spill(keeps%x1, discards%x1, lspill_list, ldestructive) call util_spill(keeps%x2, discards%x2, lspill_list, ldestructive) call util_spill(keeps%v1, discards%v1, lspill_list, ldestructive) call util_spill(keeps%v2, discards%v2, lspill_list, ldestructive) + call util_spill(keeps%t, discards%t, lspill_list, ldestructive) + + nenc_old = keeps%nenc ! This is the base class, so will be the last to be called in the cascade. ! Therefore we need to set the nenc values for both the keeps and discareds - discards%nenc = count(lspill_list(:)) - keeps%nenc = count(.not.lspill_list(:)) - if (keeps%nenc > size(keeps%status)) keeps%status(keeps%nenc+1:size(keeps%status)) = INACTIVE + discards%nenc = count(lspill_list(1:nenc_old)) + if (ldestructive) keeps%nenc = nenc_old - discards%nenc end associate return @@ -237,11 +407,8 @@ module subroutine util_spill_pl(self, discards, lspill_list, ldestructive) class(swiftest_body), intent(inout) :: discards !! Discarded object logical, dimension(:), intent(in) :: lspill_list !! Logical array of bodies to spill into the discards logical, intent(in) :: ldestructive !! Logical flag indicating whether or not this operation should alter body by removing the discard list - ! Internals - integer(I4B) :: i associate(keeps => self) - select type (discards) ! The standard requires us to select the type of both arguments in order to access all the components class is (swiftest_pl) !> Spill components specific to the massive body class @@ -258,6 +425,8 @@ module subroutine util_spill_pl(self, discards, lspill_list, ldestructive) call util_spill(keeps%Ip, discards%Ip, lspill_list, ldestructive) call util_spill(keeps%rot, discards%rot, lspill_list, ldestructive) + if (ldestructive .and. allocated(keeps%k_plpl)) deallocate(keeps%k_plpl) + call util_spill_body(keeps, discards, lspill_list, ldestructive) class default write(*,*) 'Error! spill method called for incompatible return type on swiftest_pl' diff --git a/src/util/util_valid.f90 b/src/util/util_valid.f90 index f05c81f35..eb6df7577 100644 --- a/src/util/util_valid.f90 +++ b/src/util/util_valid.f90 @@ -12,7 +12,7 @@ module subroutine util_valid_id_system(self, param) implicit none ! Arguments class(swiftest_nbody_system), intent(inout) :: self !! Swiftest nbody system object - class(swiftest_parameters), intent(in) :: param !! Current run configuration parameters + class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters ! Internals integer(I4B) :: i integer(I4B), dimension(:), allocatable :: idarr @@ -34,7 +34,7 @@ module subroutine util_valid_id_system(self, param) call util_exit(FAILURE) end if end do - self%maxid = maxval(idarr) + param%maxid = max(param%maxid, maxval(idarr)) end associate return diff --git a/src/whm/whm_kick.f90 b/src/whm/whm_kick.f90 index 2da00c332..f831ce15b 100644 --- a/src/whm/whm_kick.f90 +++ b/src/whm/whm_kick.f90 @@ -80,17 +80,17 @@ module subroutine whm_kick_getacch_tp(self, system, param, t, lbeg) system%lbeg = lbeg if (lbeg) then - ah0(:) = whm_kick_getacch_ah0(pl%Gmass(:), pl%xbeg(:,:), npl) + ah0(:) = whm_kick_getacch_ah0(pl%Gmass(1:npl), pl%xbeg(:, 1:npl), npl) do concurrent(i = 1:ntp, tp%lmask(i)) tp%ah(:, i) = tp%ah(:, i) + ah0(:) end do - call tp%accel_int(pl%Gmass(:), pl%xbeg(:,:), npl) + call tp%accel_int(pl%Gmass(1:npl), pl%xbeg(:, 1:npl), npl) else - ah0(:) = whm_kick_getacch_ah0(pl%Gmass(:), pl%xend(:,:), npl) + ah0(:) = whm_kick_getacch_ah0(pl%Gmass(1:npl), pl%xend(:, 1:npl), npl) do concurrent(i = 1:ntp, tp%lmask(i)) tp%ah(:, i) = tp%ah(:, i) + ah0(:) end do - call tp%accel_int(pl%Gmass(:), pl%xend(:,:), npl) + call tp%accel_int(pl%Gmass(1:npl), pl%xend(:, 1:npl), npl) end if if (param%loblatecb) call tp%accel_obl(system) @@ -213,13 +213,13 @@ module subroutine whm_kick_vh_pl(self, system, param, t, dt, lbeg) if (lbeg) then if (pl%lfirst) then call pl%h2j(cb) - pl%ah(:,:) = 0.0_DP + pl%ah(:, 1:npl) = 0.0_DP call pl%accel(system, param, t, lbeg) pl%lfirst = .false. end if call pl%set_beg_end(xbeg = pl%xh) else - pl%ah(:,:) = 0.0_DP + pl%ah(:, 1:npl) = 0.0_DP call pl%accel(system, param, t, lbeg) call pl%set_beg_end(xend = pl%xh) end if @@ -254,20 +254,16 @@ module subroutine whm_kick_vh_tp(self, system, param, t, dt, lbeg) associate(tp => self, ntp => self%nbody) if (tp%lfirst) then - where(tp%lmask(1:ntp)) - tp%ah(1,1:ntp) = 0.0_DP - tp%ah(2,1:ntp) = 0.0_DP - tp%ah(3,1:ntp) = 0.0_DP - end where + do concurrent(i = 1:ntp, tp%lmask(i)) + tp%ah(:, i) = 0.0_DP + end do call tp%accel(system, param, t, lbeg=.true.) tp%lfirst = .false. end if if (.not.lbeg) then - where(tp%lmask(1:ntp)) - tp%ah(1,1:ntp) = 0.0_DP - tp%ah(2,1:ntp) = 0.0_DP - tp%ah(3,1:ntp) = 0.0_DP - end where + do concurrent(i = 1:ntp, tp%lmask(i)) + tp%ah(:, i) = 0.0_DP + end do call tp%accel(system, param, t, lbeg) end if do concurrent(i = 1:ntp, tp%lmask(i)) diff --git a/src/whm/whm_setup.f90 b/src/whm/whm_setup.f90 index eaed16c14..3c5cdeec3 100644 --- a/src/whm/whm_setup.f90 +++ b/src/whm/whm_setup.f90 @@ -16,7 +16,7 @@ module subroutine whm_setup_pl(self, n, param) !> Call allocation method for parent class call setup_pl(self, n, param) - if (n <= 0) return + if (n < 0) return if (allocated(self%eta)) deallocate(self%eta) if (allocated(self%muj)) deallocate(self%muj) @@ -24,6 +24,8 @@ module subroutine whm_setup_pl(self, n, param) if (allocated(self%vj)) deallocate(self%vj) if (allocated(self%ir3j)) deallocate(self%ir3j) + if (n == 0) return + allocate(self%eta(n)) allocate(self%muj(n)) allocate(self%xj(NDIM, n)) @@ -73,13 +75,14 @@ module subroutine whm_setup_initialize_system(self, param) !! implicit none ! Arguments - class(whm_nbody_system), intent(inout) :: self !! Swiftest system object + class(whm_nbody_system), intent(inout) :: self !! WHM nbody system object class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters call setup_initialize_system(self, param) ! First we need to make sure that the massive bodies are sorted by heliocentric distance before computing jacobies call util_set_ir3h(self%pl) call self%pl%sort("ir3h", ascending=.false.) + call self%pl%index(param) ! Make sure that the discard list gets allocated initially call self%tp_discards%setup(0, param) diff --git a/src/whm/whm_util.f90 b/src/whm/whm_util.f90 index cc84ba3d5..e8ed91854 100644 --- a/src/whm/whm_util.f90 +++ b/src/whm/whm_util.f90 @@ -125,9 +125,11 @@ module subroutine whm_util_sort_pl(self, sortby, ascending) character(*), intent(in) :: sortby !! Sorting attribute logical, intent(in) :: ascending !! Logical flag indicating whether or not the sorting should be in ascending or descending order ! Internals - integer(I4B), dimension(self%nbody) :: ind + integer(I4B), dimension(:), allocatable :: ind integer(I4B) :: direction + if (self%nbody == 0) return + if (ascending) then direction = 1 else @@ -135,6 +137,7 @@ module subroutine whm_util_sort_pl(self, sortby, ascending) end if associate(pl => self, npl => self%nbody) + allocate(ind(npl)) select case(sortby) case("eta") call util_sort(direction * pl%eta(1:npl), ind(1:npl)) @@ -165,21 +168,17 @@ module subroutine whm_util_sort_rearrange_pl(self, ind) ! Arguments class(whm_pl), intent(inout) :: self !! WHM massive body object integer(I4B), dimension(:), intent(in) :: ind !! Index array used to restructure the body (should contain all 1:n index values in the desired order) - ! Internals - class(whm_pl), allocatable :: pl_sorted !! Temporary holder for sorted body - integer(I4B) :: i if (self%nbody == 0) return associate(pl => self, npl => self%nbody) + call util_sort_rearrange(pl%eta, ind, npl) + call util_sort_rearrange(pl%xj, ind, npl) + call util_sort_rearrange(pl%vj, ind, npl) + call util_sort_rearrange(pl%muj, ind, npl) + call util_sort_rearrange(pl%ir3j, ind, npl) + call util_sort_rearrange_pl(pl,ind) - allocate(pl_sorted, source=self) - if (allocated(pl%eta)) pl%eta(1:npl) = pl_sorted%eta(ind(1:npl)) - if (allocated(pl%xj)) pl%xj(:,1:npl) = pl_sorted%xj(:,ind(1:npl)) - if (allocated(pl%vj)) pl%vj(:,1:npl) = pl_sorted%vj(:,ind(1:npl)) - if (allocated(pl%muj)) pl%muj(1:npl) = pl_sorted%muj(ind(1:npl)) - if (allocated(pl%ir3j)) pl%ir3j(1:npl) = pl_sorted%ir3j(ind(1:npl)) - deallocate(pl_sorted) end associate return