"
+ ],
+ "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.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.supercatastrophic_headon.in b/examples/symba_energy_momentum/param.supercatastrophic_headon.in
index a8ff7cbde..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
@@ -17,12 +17,11 @@ CHK_RMIN 0.005
CHK_RMAX 1e6
CHK_EJECT -1.0 ! ignore this check
CHK_QMIN -1.0 ! ignore this check
-DISCARD_OUT discard.supercatastrophic_headon.out
-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
index cc62da4f4..85b99c0fa 100755
--- a/examples/symba_mars_disk/aescattermovie.py
+++ b/examples/symba_mars_disk/aescattermovie.py
@@ -13,18 +13,18 @@
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
- nframes = int(ds['time'].size / framejump)
+ 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.ds['radmarker'] = self.ds['Radius'].fillna(0)
- self.ds['radmarker'] = self.ds['radmarker'] / self.ds['radmarker'].max() * radscale
-
self.clist = {'Initial conditions' : 'xkcd:faded blue',
'Disruption' : 'xkcd:marigold',
'Supercatastrophic' : 'xkcd:shocking pink',
@@ -38,14 +38,15 @@ def __init__(self, ds, param):
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=False)
+ 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 == value
+ 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
@@ -53,7 +54,7 @@ def scatters(self, pl, radmarker, origin):
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))
# set up the figure
self.ax.margins(x=10, y=1)
@@ -62,7 +63,7 @@ def setup_plot(self):
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")
+ 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)
@@ -70,30 +71,35 @@ def setup_plot(self):
self.s1 = slist[1]
self.s2 = slist[2]
self.s3 = slist[3]
- self.ax.legend(loc='upper right')
+ 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(np.invert(np.isnan(d['a'])), drop=True)
- Radius = d['radmarker'].values
- GMass = d['GMass'].values
- a = d['a'].values / RMars
+
+ 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['id'].values
- npl = d.id.count().values
+ name = d['name'].values
+ npl = d['npl'].values[0]
radmarker = d['radmarker']
- origin = d['origin_type']
+ 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
+ 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))
+ 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")
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 447d1e308..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
-727 1.71022032e+06 2.13948145e+04 ! particle number mass Rhill
-1.24108926e+04 !particle radius in m
--8.12608230e+06 -4.37306608e+06 -9.62736144e+03 ! x y z
-9.87984575e+02 -1.88769371e+03 1.06882012e+01 ! vx vy vz
-0.4 0.4 0.4 ! Ip
-0.0 0.0 0.0 ! rot
-231 6.25152932e+05 1.58916481e+04 ! particle number mass Rhill
-8.87389776e+03 !particle radius in m
--8.21586374e+06 -4.28792953e+06 2.41010139e+04 ! x y z
-1.01581225e+03 -1.90933511e+03 -2.60449634e+00 ! vx vy vz
-0.4 0.4 0.4 ! Ip
-0.0 0.0 0.0 ! rot
-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
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-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
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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
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-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 ! Ip
0.0 0.0 0.0 ! rot
-30 7.84395275e+05 1.87003585e+04 ! particle number mass Rhill
-9.57114700e+03 !particle radius in m
+Body30 7.84395275e+05 1.87003585e+04 ! particle number mass Rhill
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7.25596696e+06 -7.23053656e+06 1.87472853e+03 ! x y z
1.43916819e+03 1.45132061e+03 9.58485615e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-31 6.50793385e+04 1.12167591e+04 ! particle number mass Rhill
-6.15153311e+03 !particle radius in m
+Body31 6.50793385e+04 1.12167591e+04 ! particle number mass Rhill
+6.15153311e+03 !particle radius in AU
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-1.50263763e+03 -8.87670849e+02 -4.72544240e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
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-1.10887000e+04 !particle radius in m
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-4.85214384e+06 9.94913086e+06 -1.36593449e+05 ! x y z
-1.77462439e+03 -8.70796881e+02 -4.04772339e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-33 6.39027490e+04 8.29271375e+03 ! particle number mass Rhill
-6.11423561e+03 !particle radius in m
+Body33 6.39027490e+04 8.29271375e+03 ! particle number mass Rhill
+6.11423561e+03 !particle radius in AU
-8.57362843e+06 -5.69257679e+06 -1.86992418e+04 ! x y z
1.16808481e+03 -1.69357760e+03 1.48289207e-01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-34 1.08790745e+05 9.99433624e+03 ! particle number mass Rhill
-4.95430775e+03 !particle radius in m
+Body34 1.08790745e+05 9.99433624e+03 ! particle number mass Rhill
+4.95430775e+03 !particle radius in AU
-1.19543227e+04 1.04662309e+07 -2.75529146e+04 ! x y z
-2.03252516e+03 -1.02408335e+01 -9.64298816e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-35 8.08651729e+05 1.70555918e+04 ! particle number mass Rhill
-9.66880578e+03 !particle radius in m
+Body35 8.08651729e+05 1.70555918e+04 ! particle number mass Rhill
+9.66880578e+03 !particle radius in AU
-1.68361528e+06 9.15840339e+06 -9.34661786e+04 ! x y z
-2.10432868e+03 -3.67110160e+02 2.17992849e+01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-36 5.50682707e+05 1.64680955e+04 ! particle number mass Rhill
-8.50653728e+03 !particle radius in m
+Body36 5.50682707e+05 1.64680955e+04 ! particle number mass Rhill
+8.50653728e+03 !particle radius in AU
7.61819019e+06 6.79194080e+06 -4.97100639e+04 ! x y z
-1.37259731e+03 1.51157244e+03 2.28319862e+01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-37 1.31696234e+06 2.34161781e+04 ! particle number mass Rhill
-1.13756647e+04 !particle radius in m
+Body37 1.31696234e+06 2.34161781e+04 ! particle number mass Rhill
+1.13756647e+04 !particle radius in AU
-8.27002578e+05 -1.07584936e+07 -8.18905340e+04 ! x y z
1.98624835e+03 -1.45613526e+02 -2.22634090e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.0 0.0 0.0 ! rot
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0.4 0.4 0.4 ! Ip
diff --git a/examples/symba_mars_disk/param.in b/examples/symba_mars_disk/param.in
index 13f933aa7..1fac92462 100644
--- a/examples/symba_mars_disk/param.in
+++ b/examples/symba_mars_disk/param.in
@@ -1,17 +1,17 @@
!Parameter file for the SyMBA-RINGMOONS test
T0 0.0
-TSTOP 100000000.0
+TSTOP 1.0e12
DT 600.0
CB_IN cb.in
PL_IN mars.in
TP_IN tp.in
IN_TYPE ASCII
-ISTEP_OUT 10
-ISTEP_DUMP 10
-BIN_OUT bin.dat
+ISTEP_OUT 1
+ISTEP_DUMP 1
+BIN_OUT bin.nc
PARTICLE_OUT particle.dat
-OUT_TYPE REAL8
-OUT_FORM EL
+OUT_TYPE NETCDF_DOUBLE
+OUT_FORM XVEL
OUT_STAT REPLACE
CHK_CLOSE yes
CHK_RMIN 3389500.0
@@ -21,9 +21,9 @@ 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
+GMTINY 10000.0
+MIN_GMFRAG 1000.0
ENERGY yes
FRAGMENTATION yes
ROTATION yes
@@ -31,5 +31,3 @@ MU2KG 1.0
DU2M 1.0
TU2S 1.0
SEED 2 3080983 2220830
-DISCARD_OUT discard.out
-ENERGY_OUT energy.out
diff --git a/examples/symba_mars_disk/runswiftest.sh b/examples/symba_mars_disk/runswiftest.sh
new file mode 100644
index 000000000..c7d069d39
--- /dev/null
+++ b/examples/symba_mars_disk/runswiftest.sh
@@ -0,0 +1,34 @@
+#!/bin/zsh -l
+#SBATCH -A daminton
+#SBATCH --nodes=1
+#SBATCH --ntasks=1
+#SBATCH --time=14-00:00:00
+#SBATCH --ntasks-per-node=1
+#SBATCH --cpus-per-task=4
+#SBATCH --mem-per-cpu=1G
+#SBATCH --job-name=high_high
+#SBATCH --no-requeue
+#SBATCH -o %x.out
+#SBATCH -e %x.err
+cd $SLURM_SUBMIT_DIR
+
+module load utilities monitor
+#module load gcc/10.2.0
+#netcdf-fortran/4.5.3
+
+# track per-code CPU load
+monitor cpu percent --all-cores >cpu-percent.log &
+CPU_PID=$!
+
+# track memory usage
+monitor cpu memory >cpu-memory.log &
+MEM_PID=$!
+
+
+export OMP_NUM_THREADS=12
+export KMP_STACKSIZE=2G
+./swiftest_driver symba param.in
+
+# shut down the resource monitors
+kill -s INT $CPU_PID $MEM_PID
+
diff --git a/examples/symba_mars_disk/testnetcdf.ipynb b/examples/symba_mars_disk/testnetcdf.ipynb
new file mode 100644
index 000000000..be4bf6a11
--- /dev/null
+++ b/examples/symba_mars_disk/testnetcdf.ipynb
@@ -0,0 +1,6197 @@
+{
+ "cells": [
+ {
+ "cell_type": "code",
+ "execution_count": 1,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "text/plain": [
+ "'/home/daminton/git/swiftest/examples/symba_mars_disk'"
+ ]
+ },
+ "execution_count": 1,
+ "metadata": {},
+ "output_type": "execute_result"
+ }
+ ],
+ "source": [
+ "import swiftest\n",
+ "import os\n",
+ "import xarray as xr\n",
+ "import numpy as np\n",
+ "os.getcwd()"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 2,
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "Reading Swiftest file param.in\n",
+ "\n",
+ "Creating Dataset\n",
+ "Successfully converted 6 output frames.\n",
+ "Swiftest simulation data stored as xarray DataSet .ds\n"
+ ]
+ }
+ ],
+ "source": [
+ "sim = swiftest.Simulation(param_file=\"param.in\")\n",
+ "sim.bin2xr()\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 3,
+ "metadata": {},
+ "outputs": [
+ {
+ "data": {
+ "text/html": [
+ "
"
+ ],
+ "text/plain": [
+ "\n",
+ "Dimensions: ()\n",
+ "Coordinates:\n",
+ " id int32 2\n",
+ "Data variables: (12/57)\n",
+ " npl float64 1.518e+03\n",
+ " ntp float64 0.0\n",
+ " name object 'Body3'\n",
+ " particle_type object 'Massive Body'\n",
+ " xhx float64 -3.025e+06\n",
+ " xhy float64 -1.02e+07\n",
+ " ... ...\n",
+ " discard_xhy float64 0.0\n",
+ " discard_xhz float64 0.0\n",
+ " discard_vhx float64 0.0\n",
+ " discard_vhy float64 2.122e-314\n",
+ " discard_vhz float64 3.024e-153\n",
+ " discard_body_id float64 -2.147e+09"
+ ]
+ },
+ "execution_count": 22,
+ "metadata": {},
+ "output_type": "execute_result"
+ }
+ ],
+ "source": [
+ "lastframe.sel(id=2)"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "metadata": {},
+ "outputs": [],
+ "source": []
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "swiftestOOF",
+ "language": "python",
+ "name": "swiftestoof"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 3
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython3",
+ "version": "3.7.10"
+ }
+ },
+ "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_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_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/mars_disk/pl.swifter.in b/examples/symba_swifter_comparison/mars_disk/pl.swifter.in
index 09a72ef61..4c31c52c1 100644
--- a/examples/symba_swifter_comparison/mars_disk/pl.swifter.in
+++ b/examples/symba_swifter_comparison/mars_disk/pl.swifter.in
@@ -2,6003 +2,6003 @@
1 4.28388662e+13
.0 .0 .0 ! x y z
.0 .0 .0 !vx vy vz
-727 1.71022032e+06 2.13948145e+04 ! particle number mass Rhill
+727 1.71022032e+06 2.13948145e+04 ! particle number mass rhill
1.24108926e+04 !particle radius in m
-8.12608230e+06 -4.37306608e+06 -9.62736144e+03 ! x y z
9.87984575e+02 -1.88769371e+03 1.06882012e+01 ! vx vy vz
-231 6.25152932e+05 1.58916481e+04 ! particle number mass Rhill
+231 6.25152932e+05 1.58916481e+04 ! particle number mass rhill
8.87389776e+03 !particle radius in m
-8.21586374e+06 -4.28792953e+06 2.41010139e+04 ! x y z
1.01581225e+03 -1.90933511e+03 -2.60449634e+00 ! vx vy vz
-2 9.90685589e+04 8.35558297e+03 ! particle number mass Rhill
+2 9.90685589e+04 8.35558297e+03 ! particle number mass rhill
7.07643092e+03 !particle radius in m
-2.35807426e+06 8.60445552e+06 1.25224401e+04 ! x y z
-2.13373621e+03 -5.91159549e+02 -1.46482980e+00 ! vx vy vz
-3 3.17438752e+04 6.69500494e+03 ! particle number mass Rhill
+3 3.17438752e+04 6.69500494e+03 ! particle number mass rhill
4.84234399e+03 !particle radius in m
-8.01160007e+06 -6.93642997e+06 1.51456130e+04 ! x y z
1.31205897e+03 -1.53256580e+03 -1.41252951e-01 ! vx vy vz
-4 3.98556011e+05 1.56022902e+04 ! particle number mass Rhill
+4 3.98556011e+05 1.56022902e+04 ! particle number mass rhill
1.12546530e+04 !particle radius in m
8.10802666e+05 1.07743901e+07 2.02908991e+04 ! x y z
-1.97583939e+03 1.47020293e+02 2.81847341e-01 ! vx vy vz
-5 1.44988335e+05 1.52187807e+04 ! particle number mass Rhill
+5 1.44988335e+05 1.52187807e+04 ! particle number mass rhill
5.45209420e+03 !particle radius in m
1.19634122e+07 -8.10716246e+06 -5.95532256e+04 ! x y z
9.82512278e+02 1.42576317e+03 8.88854207e+00 ! vx vy vz
-6 3.78500932e+05 1.43710361e+04 ! particle number mass Rhill
+6 3.78500932e+05 1.43710361e+04 ! particle number mass rhill
7.50714229e+03 !particle radius in m
-9.39611249e+06 3.86341011e+06 4.12677461e+04 ! x y z
-8.05714130e+02 -1.87378063e+03 1.44571432e+01 ! vx vy vz
-7 4.22792487e+05 1.91833939e+04 ! particle number mass Rhill
+7 4.22792487e+05 1.91833939e+04 ! particle number mass rhill
7.78923399e+03 !particle radius in m
-4.75251420e+06 -1.21243281e+07 -4.63584868e+04 ! x y z
1.67483168e+03 -6.72935315e+02 -2.51894419e+00 ! vx vy vz
-8 7.71745838e+05 2.46689817e+04 ! particle number mass Rhill
+8 7.71745838e+05 2.46689817e+04 ! particle number mass rhill
9.51941869e+03 !particle radius in m
-1.85450966e+06 -1.34716389e+07 8.25492639e+04 ! x y z
1.75187299e+03 -2.73602528e+02 -3.13786565e+00 ! vx vy vz
-9 9.61893115e+05 2.40394481e+04 ! particle number mass Rhill
+9 9.61893115e+05 2.40394481e+04 ! particle number mass rhill
1.02445905e+04 !particle radius in m
1.23514674e+07 2.68920661e+05 1.39262437e+04 ! x y z
-5.46299990e+01 1.85637492e+03 8.88156878e+00 ! vx vy vz
-10 9.05777402e+05 1.85084324e+04 ! particle number mass Rhill
+10 9.05777402e+05 1.85084324e+04 ! particle number mass rhill
1.00413666e+04 !particle radius in m
-3.23931710e+06 -9.01689172e+06 -4.12799209e+04 ! x y z
2.01018172e+03 -6.80970287e+02 7.47887585e+00 ! vx vy vz
-11 7.45490873e+05 1.85936744e+04 ! particle number mass Rhill
+11 7.45490873e+05 1.85936744e+04 ! particle number mass rhill
9.41021993e+03 !particle radius in m
-8.22383274e+06 6.53912283e+06 -4.14927827e+04 ! x y z
-1.24361728e+03 -1.57101590e+03 1.15408315e+01 ! vx vy vz
-12 1.62561944e+05 1.74719338e+04 ! particle number mass Rhill
+12 1.62561944e+05 1.74719338e+04 ! particle number mass rhill
5.66402670e+03 !particle radius in m
1.08162501e+06 1.60434368e+07 -1.90513596e+05 ! x y z
-1.63320995e+03 9.41371249e+01 -1.08583324e+00 ! vx vy vz
-13 2.53914705e+05 1.18629878e+04 ! particle number mass Rhill
+13 2.53914705e+05 1.18629878e+04 ! particle number mass rhill
9.68422654e+03 !particle radius in m
8.87638562e+06 -3.42494393e+06 3.77051239e+04 ! x y z
7.17031490e+02 1.98991002e+03 1.65715407e+00 ! vx vy vz
-14 4.49497062e+05 1.80709533e+04 ! particle number mass Rhill
+14 4.49497062e+05 1.80709533e+04 ! particle number mass rhill
1.17150625e+04 !particle radius in m
8.43240423e+06 -8.47557599e+06 9.53685695e+04 ! x y z
1.37244856e+03 1.29766742e+03 6.52389482e-01 ! vx vy vz
-15 1.26801801e+06 2.59747860e+04 ! particle number mass Rhill
+15 1.26801801e+06 2.59747860e+04 ! particle number mass rhill
1.12329581e+04 !particle radius in m
9.22664947e+06 8.30989011e+06 -5.74831096e+04 ! x y z
-1.25111883e+03 1.34059241e+03 8.55955292e+00 ! vx vy vz
-16 9.75352347e+05 2.91597894e+04 ! particle number mass Rhill
+16 9.75352347e+05 2.91597894e+04 ! particle number mass rhill
1.02921516e+04 !particle radius in m
-4.08982641e+06 1.42813091e+07 2.62466604e+04 ! x y z
-1.63050329e+03 -4.70983328e+02 5.42658810e+00 ! vx vy vz
-17 5.40910752e+04 7.00056187e+03 ! particle number mass Rhill
+17 5.40910752e+04 7.00056187e+03 ! particle number mass rhill
3.92489041e+03 !particle radius in m
8.28836769e+06 -4.56966319e+06 -1.00925184e+04 ! x y z
1.01075458e+03 1.85603564e+03 9.12767608e-01 ! vx vy vz
-18 1.99689612e+06 3.23933078e+04 ! particle number mass Rhill
+18 1.99689612e+06 3.23933078e+04 ! particle number mass rhill
1.30688534e+04 !particle radius in m
-7.36104027e+06 -1.05891946e+07 7.75267384e+04 ! x y z
1.50650168e+03 -1.03626339e+03 6.92830281e+00 ! vx vy vz
-19 1.15056094e+06 2.84099265e+04 ! particle number mass Rhill
+19 1.15056094e+06 2.84099265e+04 ! particle number mass rhill
1.08748232e+04 !particle radius in m
-1.16432549e+07 7.04896042e+06 1.31826777e+04 ! x y z
-9.22639859e+02 -1.52066967e+03 -1.15982407e+01 ! vx vy vz
-20 9.02282771e+04 1.44052969e+04 ! particle number mass Rhill
+20 9.02282771e+04 1.44052969e+04 ! particle number mass rhill
4.65478777e+03 !particle radius in m
1.54278872e+07 -4.66477914e+06 2.89150511e+04 ! x y z
4.74802657e+02 1.56436208e+03 1.16558658e+00 ! vx vy vz
-21 2.52706341e+05 1.13089015e+04 ! particle number mass Rhill
+21 2.52706341e+05 1.13089015e+04 ! particle number mass rhill
6.56131734e+03 !particle radius in m
8.25405514e+06 -3.99894087e+06 -1.03017471e+05 ! x y z
9.55530709e+02 1.91876743e+03 -2.12478228e+01 ! vx vy vz
-22 3.44014800e+05 1.39895248e+04 ! particle number mass Rhill
+22 3.44014800e+05 1.39895248e+04 ! particle number mass rhill
7.27184654e+03 !particle radius in m
-1.01048660e+07 -7.25267430e+05 3.72763878e+04 ! x y z
1.50338830e+02 -2.04513843e+03 -6.64737882e+00 ! vx vy vz
-23 2.72301402e+04 6.52734935e+03 ! particle number mass Rhill
+23 2.72301402e+04 6.52734935e+03 ! particle number mass rhill
4.60100051e+03 !particle radius in m
1.08085981e+07 8.91343848e+05 -8.59837690e+04 ! x y z
-1.73598988e+02 1.98921090e+03 7.39675166e+00 ! vx vy vz
-24 1.88387060e+06 4.79739567e+04 ! particle number mass Rhill
+24 1.88387060e+06 4.79739567e+04 ! particle number mass rhill
1.28174811e+04 !particle radius in m
-1.95760874e+07 2.13874411e+06 9.87141675e+04 ! x y z
-1.78019032e+02 -1.46067517e+03 7.47552271e+00 ! vx vy vz
-25 1.99552106e+06 3.51994254e+04 ! particle number mass Rhill
+25 1.99552106e+06 3.51994254e+04 ! particle number mass rhill
1.30658530e+04 !particle radius in m
-5.15587895e+06 1.31093030e+07 2.34999443e+04 ! x y z
-1.60915655e+03 -6.75665775e+02 -1.41401807e-02 ! vx vy vz
-26 9.80460627e+05 2.82973543e+04 ! particle number mass Rhill
+26 9.80460627e+05 2.82973543e+04 ! particle number mass rhill
1.03100883e+04 !particle radius in m
-1.04206598e+07 1.04694469e+07 3.71773715e+04 ! x y z
-1.22193412e+03 -1.15184993e+03 -7.42970615e+00 ! vx vy vz
-27 2.99657072e+05 1.52153060e+04 ! particle number mass Rhill
+27 2.99657072e+05 1.52153060e+04 ! particle number mass rhill
1.02339628e+04 !particle radius in m
-8.37104048e+06 -7.31013791e+06 1.37822827e+05 ! x y z
1.31083458e+03 -1.50225202e+03 1.24188931e+01 ! vx vy vz
-28 5.82137831e+05 2.49711445e+04 ! particle number mass Rhill
+28 5.82137831e+05 2.49711445e+04 ! particle number mass rhill
8.66551286e+03 !particle radius in m
-1.37026179e+07 6.52187486e+06 4.74483726e+04 ! x y z
-7.21171063e+02 -1.51233609e+03 4.06777653e+00 ! vx vy vz
-29 1.10612525e+06 1.96262714e+04 ! particle number mass Rhill
+29 1.10612525e+06 1.96262714e+04 ! particle number mass rhill
1.07329828e+04 !particle radius in m
7.27063487e+05 9.63835599e+06 7.97365647e+04 ! x y z
-2.09031891e+03 1.45245810e+02 -8.30488647e+00 ! vx vy vz
-30 7.84395275e+05 1.87003585e+04 ! particle number mass Rhill
+30 7.84395275e+05 1.87003585e+04 ! particle number mass rhill
9.57114700e+03 !particle radius in m
7.25596696e+06 -7.23053656e+06 1.87472853e+03 ! x y z
1.43916819e+03 1.45132061e+03 9.58485615e+00 ! vx vy vz
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diff --git a/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in b/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in
index 447d1e308..72a58d839 100644
--- a/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in
+++ b/examples/symba_swifter_comparison/mars_disk/pl.swiftest.in
@@ -1,8999 +1,8999 @@
1500 ! Mars System in SI units
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0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
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0.4 0.4 0.4 ! Ip
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1.07221971e+04 !particle radius in m
-1.31449667e+07 5.65642590e+06 -1.35348879e+04 ! x y z
-6.99474388e+02 -1.58839301e+03 5.07187025e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1489 9.64986931e+05 2.60335138e+04 ! particle number mass Rhill
+1489 9.64986931e+05 2.60335138e+04 ! particle number mass rhill
1.02555622e+04 !particle radius in m
-1.28107010e+07 3.64301270e+06 -4.79094708e+04 ! x y z
-4.96849501e+02 -1.72146269e+03 1.99970261e+01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1490 3.85017463e+05 1.31518104e+04 ! particle number mass Rhill
+1490 3.85017463e+05 1.31518104e+04 ! particle number mass rhill
7.54998008e+03 !particle radius in m
-8.81052520e+06 1.96363775e+06 -7.03542162e+04 ! x y z
-4.55600237e+02 -2.14195252e+03 -1.54510587e+01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1491 7.12464696e+04 7.27507090e+03 ! particle number mass Rhill
+1491 7.12464696e+04 7.27507090e+03 ! particle number mass rhill
4.30236032e+03 !particle radius in m
6.76054921e+06 5.69153857e+06 -8.32813680e+04 ! x y z
-1.43863210e+03 1.66962801e+03 -3.05680786e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1492 2.30337841e+05 1.99962209e+04 ! particle number mass Rhill
+1492 2.30337841e+05 1.99962209e+04 ! particle number mass rhill
9.37470089e+03 !particle radius in m
-1.58533753e+07 -4.64141565e+06 -1.37616342e+05 ! x y z
4.71661565e+02 -1.53679456e+03 4.54920894e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1493 1.54078080e+05 1.40811002e+04 ! particle number mass Rhill
+1493 1.54078080e+05 1.40811002e+04 ! particle number mass rhill
5.56372876e+03 !particle radius in m
-5.05912024e+06 1.20461614e+07 -1.00213774e+05 ! x y z
-1.67920042e+03 -7.11202226e+02 4.13175962e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1494 8.27228641e+04 9.01203219e+03 ! particle number mass Rhill
+1494 8.27228641e+04 9.01203219e+03 ! particle number mass rhill
6.66362952e+03 !particle radius in m
8.41034459e+05 -1.03591089e+07 -4.26263251e+04 ! x y z
2.02679172e+03 1.77245292e+02 -7.59374588e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1495 6.59711957e+04 7.21319042e+03 ! particle number mass Rhill
+1495 6.59711957e+04 7.21319042e+03 ! particle number mass rhill
4.19344015e+03 !particle radius in m
-8.72674150e+06 -1.84604826e+06 -9.49439666e+03 ! x y z
5.06255038e+02 -2.14329601e+03 8.35004981e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1496 4.76016816e+05 1.56977540e+04 ! particle number mass Rhill
+1496 4.76016816e+05 1.56977540e+04 ! particle number mass rhill
1.19410657e+04 !particle radius in m
8.32975138e+06 5.59994962e+06 1.36490477e+04 ! x y z
-1.14500563e+03 1.73284125e+03 2.21368330e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1497 8.74132422e+05 1.84842648e+04 ! particle number mass Rhill
+1497 8.74132422e+05 1.84842648e+04 ! particle number mass rhill
9.92303995e+03 !particle radius in m
5.20187427e+06 8.26928364e+06 7.79156795e+04 ! x y z
-1.78869520e+03 1.08594628e+03 -2.89543422e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1498 1.05100593e+06 1.88653392e+04 ! particle number mass Rhill
+1498 1.05100593e+06 1.88653392e+04 ! particle number mass rhill
1.05516583e+04 !particle radius in m
-3.97296892e+06 -8.38171851e+06 1.59358464e+04 ! x y z
1.95617296e+03 -9.13960827e+02 -3.62965884e-01 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1499 4.64374943e+05 2.44967912e+04 ! particle number mass Rhill
+1499 4.64374943e+05 2.44967912e+04 ! particle number mass rhill
8.03665372e+03 !particle radius in m
8.20764080e+05 -1.58893023e+07 7.87114038e+04 ! x y z
1.64101205e+03 9.20364252e+01 9.68548448e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1500 7.98550448e+05 3.23468692e+04 ! particle number mass Rhill
+1500 7.98550448e+05 3.23468692e+04 ! particle number mass rhill
9.62837764e+03 !particle radius in m
-9.69224879e+06 1.49532038e+07 7.33593405e+04 ! x y z
-1.29931651e+03 -8.27698792e+02 -3.16602237e+00 ! vx vy vz
0.4 0.4 0.4 ! Ip
0.0 0.0 0.0 ! rot
-1501 7.54058320e+04 8.18405513e+03 ! particle number mass Rhill
+1501 7.54058320e+04 8.18405513e+03 ! particle number mass rhill
4.38450573e+03 !particle radius in m
-5.62663613e+06 7.91766436e+06 2.60207243e+04 ! x y z
-1.74178290e+03 -1.18522553e+03 2.27430689e+00 ! vx vy vz
diff --git a/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb b/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb
index 96c456367..1dca7f7e8 100644
--- a/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb
+++ b/examples/symba_swifter_comparison/mars_disk/swiftest_vs_swifter.ipynb
@@ -43,9 +43,9 @@
"output_type": "stream",
"text": [
"Reading Swiftest file param.swiftest.in\n",
- "Reading in time 4.200e+03\n",
+ "Reading in time 0.000e+00\n",
"Creating Dataset\n",
- "Successfully converted 8 output frames.\n",
+ "Successfully converted 1 output frames.\n",
"\n",
"Adding particle info to Dataset\n",
"Swiftest simulation data stored as xarray DataSet .ds\n"
@@ -59,75 +59,7 @@
},
{
"cell_type": "code",
- "execution_count": 4,
- "metadata": {},
- "outputs": [],
- "source": [
- "swiftdiff = swiftestsim.ds - swiftersim.ds"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 5,
- "metadata": {},
- "outputs": [
- {
- "name": "stderr",
- "output_type": "stream",
- "text": [
- "No handles with labels found to put in legend.\n"
- ]
- },
- {
- "data": {
- "image/png": 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\n",
- "text/plain": [
- ""
- ]
- },
- "metadata": {
- "needs_background": "light"
- },
- "output_type": "display_data"
- },
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "\n"
- ]
- }
- ],
- "source": [
- "fig, ax = plt.subplots()\n",
- "swiftdiff['vz'].plot.line(ax=ax, x=\"time\")\n",
- "legend = ax.legend()\n",
- "legend.remove()\n",
- "plt.show()\n",
- "print(\"\")"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 20,
- "metadata": {},
- "outputs": [],
- "source": [
- "last = swiftdiff.isel(time=1)"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 21,
- "metadata": {},
- "outputs": [],
- "source": [
- "badval = last.where(last['pz'] != 0, drop=True)"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 23,
+ "execution_count": 8,
"metadata": {},
"outputs": [
{
@@ -485,429 +417,71 @@
" fill: currentColor;\n",
"}\n",
"