diff --git a/Makefile b/Makefile
index 9bda6503a..dfc6fd5c0 100644
--- a/Makefile
+++ b/Makefile
@@ -86,7 +86,7 @@ lib:
 	  ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \
 	  ln -s $(SWIFTEST_HOME)/Makefile .; \
 	  make libdir
-	cd $(SWIFTEST_HOME)/src/driftkick; \
+	cd $(SWIFTEST_HOME)/src/drift; \
 	  rm -f Makefile.Defines Makefile; \
 	  ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \
 	  ln -s $(SWIFTEST_HOME)/Makefile .; \
@@ -106,6 +106,11 @@ lib:
 	  ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \
 	  ln -s $(SWIFTEST_HOME)/Makefile .; \
 	  make libdir
+	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/obl; \
 	  rm -f Makefile.Defines Makefile; \
 	  ln -s $(SWIFTEST_HOME)/Makefile.Defines .; \
@@ -179,20 +184,21 @@ bin: *.f90
 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/driftkick;   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/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/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*
+	cd $(SWIFTEST_HOME)/src/rmvs;    rm -f Makefile.Defines Makefile *.gc*
 	cd $(SWIFTEST_HOME)/src/setup;   rm -f Makefile.Defines Makefile *.gc*
-	cd $(SWIFTEST_HOME)/src/util;    rm -f Makefile.Defines Makefile *.gc*
 	cd $(SWIFTEST_HOME)/src/user;    rm -f Makefile.Defines Makefile *.gc*
-	cd $(SWIFTEST_HOME)/src/main;    rm -f Makefile.Defines Makefile *.gc*
+	cd $(SWIFTEST_HOME)/src/util;    rm -f Makefile.Defines Makefile *.gc*
 	cd $(SWIFTEST_HOME)/src/whm;    rm -f Makefile.Defines Makefile *.gc*
-	cd $(SWIFTEST_HOME)/src/rmvs;    rm -f Makefile.Defines Makefile *.gc*
-	cd $(SWIFTEST_HOME)/src/helio;    rm -f Makefile.Defines Makefile *.gc*
 	cd $(SWIFTEST_HOME)/bin;     rm -f swiftest_*
 	cd $(SWIFTEST_HOME)/bin;     rm -f tool_*
 	cd $(SWIFTEST_HOME)/lib;     rm -f lib*
diff --git a/Makefile.Defines b/Makefile.Defines
index 820ad6d7d..07126f842 100644
--- a/Makefile.Defines
+++ b/Makefile.Defines
@@ -65,8 +65,8 @@ GPAR = -fopenmp -ftree-parallelize-loops=4
 GMEM = -fsanitize=undefined -fsanitize=address -fsanitize=leak 
 GWARNINGS = -Wall -Warray-bounds  -Wimplicit-interface -Wextra -Warray-temporaries
 
-#FFLAGS  = $(IDEBUG) $(HEAPARR)
-FFLAGS  = -init=snan,arrays -no-wrap-margin -O3 $(STRICTREAL) $(SIMDVEC) $(PAR) 
+FFLAGS  = $(IDEBUG) $(HEAPARR)
+#FFLAGS  = -init=snan,arrays -no-wrap-margin -O3 $(STRICTREAL) $(SIMDVEC) $(PAR) 
 FORTRAN = ifort
 #AR     = xiar
 
diff --git a/examples/rmvs_swifter_comparison/9pl_18tp_encounters/param.swifter.in b/examples/rmvs_swifter_comparison/9pl_18tp_encounters/param.swifter.in
index 25267812a..ec31caa63 100644
--- a/examples/rmvs_swifter_comparison/9pl_18tp_encounters/param.swifter.in
+++ b/examples/rmvs_swifter_comparison/9pl_18tp_encounters/param.swifter.in
@@ -11,8 +11,8 @@ BIN_OUT       bin.swifter.dat
 OUT_TYPE      REAL8
 OUT_FORM      XV
 OUT_STAT      UNKNOWN
-J2            0.0
-J4            0.0
+J2            4.7535806948127355e-12
+J4            -2.2473967953572827e-18
 CHK_CLOSE     yes
 CHK_RMIN      0.004650467260962157
 CHK_RMAX      1000.0
diff --git a/examples/rmvs_swifter_comparison/9pl_18tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb b/examples/rmvs_swifter_comparison/9pl_18tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb
index 304a0c190..0a95cb75e 100644
--- a/examples/rmvs_swifter_comparison/9pl_18tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb
+++ b/examples/rmvs_swifter_comparison/9pl_18tp_encounters/swiftest_rmvs_vs_swifter_rmvs.ipynb
@@ -22,13 +22,16 @@
      "output_type": "stream",
      "text": [
       "Reading Swifter file param.swifter.in\n",
+      "Reading in time 3.660e+02\n",
+      "Creating Dataset\n",
+      "Successfully converted 367 output frames.\n",
       "Swifter simulation data stored as xarray DataSet .ds\n"
      ]
     }
    ],
    "source": [
     "inparfile = 'param.swifter.in'\n",
-    "swiftersim = swiftest.Simulation(source=inparfile, codename=\"Swifter\")\n",
+    "swiftersim = swiftest.Simulation(param_file=inparfile, codename=\"Swifter\")\n",
     "swiftersim.bin2xr()\n",
     "swifterdat = swiftersim.ds"
    ]
@@ -43,13 +46,16 @@
      "output_type": "stream",
      "text": [
       "Reading Swiftest file param.swiftest.in\n",
+      "Reading in time 3.660e+02\n",
+      "Creating Dataset\n",
+      "Successfully converted 367 output frames.\n",
       "Swiftest simulation data stored as xarray DataSet .ds\n"
      ]
     }
    ],
    "source": [
     "inparfile = 'param.swiftest.in'\n",
-    "swiftestsim = swiftest.Simulation(source=inparfile)\n",
+    "swiftestsim = swiftest.Simulation(param_file=inparfile)\n",
     "swiftestsim.bin2xr()\n",
     "swiftestdat = swiftestsim.ds"
    ]
@@ -451,138 +457,81 @@
        "  stroke: currentColor;\n",
        "  fill: currentColor;\n",
        "}\n",
-       "</style><pre class='xr-text-repr-fallback'>&lt;xarray.DataArray &#x27;px&#x27; (time (d): 366)&gt;\n",
-       "array([0.00000000e+00, 2.22044605e-16, 4.44089210e-16, 8.88178420e-16,\n",
-       "       1.55431223e-15, 2.66453526e-15, 3.99680289e-15, 5.55111512e-15,\n",
-       "       7.32747196e-15, 9.32587341e-15, 1.13242749e-14, 1.35447209e-14,\n",
-       "       1.62092562e-14, 1.90958360e-14, 2.22044605e-14, 2.55351296e-14,\n",
-       "       2.90878432e-14, 3.28626015e-14, 3.68594044e-14, 4.13002965e-14,\n",
-       "       4.59632332e-14, 5.08482145e-14, 5.59552404e-14, 6.12843110e-14,\n",
-       "       6.68354261e-14, 7.26085858e-14, 7.86037901e-14, 8.50430837e-14,\n",
-       "       9.17044218e-14, 9.85878046e-14, 1.05693232e-13, 1.13242749e-13,\n",
-       "       1.20792265e-13, 1.28563826e-13, 1.36779477e-13, 1.45217172e-13,\n",
-       "       1.53876911e-13, 1.62980740e-13, 1.72528658e-13, 1.81854531e-13,\n",
-       "       1.91624494e-13, 2.01838546e-13, 2.12274642e-13, 2.22932783e-13,\n",
-       "       2.33812969e-13, 2.45137244e-13, 2.56905608e-13, 2.68896017e-13,\n",
-       "       2.81108470e-13, 2.93765012e-13, 3.06643599e-13, 3.19744231e-13,\n",
-       "       3.33066907e-13, 3.46611628e-13, 3.60822483e-13, 3.75477427e-13,\n",
-       "       3.90132371e-13, 4.05231404e-13, 4.20774526e-13, 4.36761738e-13,\n",
-       "       4.52748949e-13, 4.69180250e-13, 4.86277685e-13, 5.03153075e-13,\n",
-       "       5.20472554e-13, 5.37792033e-13, 5.55999691e-13, 5.74651438e-13,\n",
-       "       5.93525229e-13, 6.12843110e-13, 6.32827124e-13, 6.52811138e-13,\n",
-       "       6.73017198e-13, 6.93223257e-13, 7.14317494e-13, 7.36077865e-13,\n",
-       "       7.57838237e-13, 7.79820652e-13, 8.02691247e-13, 8.25561841e-13,\n",
-       "...\n",
-       "       1.31983313e-11, 1.32187594e-11, 1.32370226e-11, 1.32530653e-11,\n",
-       "       1.32669986e-11, 1.32788225e-11, 1.32883704e-11, 1.32956424e-11,\n",
-       "       1.33005829e-11, 1.33031919e-11, 1.33035249e-11, 1.33012490e-11,\n",
-       "       1.32966971e-11, 1.32894806e-11, 1.32797107e-11, 1.32676092e-11,\n",
-       "       1.32526212e-11, 1.32353017e-11, 1.32149847e-11, 1.31921141e-11,\n",
-       "       1.31665789e-11, 1.31382683e-11, 1.31069600e-11, 1.30728761e-11,\n",
-       "       1.30360167e-11, 1.29962707e-11, 1.29535271e-11, 1.29078970e-11,\n",
-       "       1.28593802e-11, 1.28074218e-11, 1.27525768e-11, 1.26949562e-11,\n",
-       "       1.26338939e-11, 1.25698341e-11, 1.25023325e-11, 1.24318333e-11,\n",
-       "       1.23581145e-11, 1.22810651e-11, 1.22007959e-11, 1.21171961e-11,\n",
-       "       1.20300436e-11, 1.19397825e-11, 1.18460797e-11, 1.17490462e-11,\n",
-       "       1.16484600e-11, 1.15446541e-11, 1.14370735e-11, 1.13261622e-11,\n",
-       "       1.12119203e-11, 1.10941256e-11, 1.09725562e-11, 1.08476561e-11,\n",
-       "       1.07189813e-11, 1.05870868e-11, 1.04514175e-11, 1.03119735e-11,\n",
-       "       1.01691988e-11, 1.00233155e-11, 9.87299131e-12, 9.71933645e-12,\n",
-       "       9.56190682e-12, 9.40092448e-12, 9.23616739e-12, 9.06807962e-12,\n",
-       "       8.89599505e-12, 8.72013572e-12, 8.54050164e-12, 8.35753688e-12,\n",
-       "       8.17101942e-12, 7.98094923e-12, 7.78666021e-12, 7.58904051e-12,\n",
-       "       7.38742401e-12, 7.18247684e-12, 6.97397695e-12, 6.76170231e-12,\n",
-       "       6.54609700e-12, 6.32649488e-12])\n",
+       "</style><pre class='xr-text-repr-fallback'>&lt;xarray.DataArray &#x27;px&#x27; (time (d): 367)&gt;\n",
+       "array([0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0.])\n",
        "Coordinates:\n",
        "    id        int64 4\n",
-       "  * time (d)  (time (d)) float64 0.0 1.0 2.0 3.0 4.0 ... 362.0 363.0 364.0 365.0</pre><div class='xr-wrap' hidden><div class='xr-header'><div class='xr-obj-type'>xarray.DataArray</div><div class='xr-array-name'>'px'</div><ul class='xr-dim-list'><li><span class='xr-has-index'>time (d)</span>: 366</li></ul></div><ul class='xr-sections'><li class='xr-section-item'><div class='xr-array-wrap'><input id='section-ebc0144f-3e8f-4ef6-a58e-17f2fbf26875' class='xr-array-in' type='checkbox' checked><label for='section-ebc0144f-3e8f-4ef6-a58e-17f2fbf26875' title='Show/hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-array-preview xr-preview'><span>0.0 2.22e-16 4.441e-16 8.882e-16 ... 6.762e-12 6.546e-12 6.326e-12</span></div><div class='xr-array-data'><pre>array([0.00000000e+00, 2.22044605e-16, 4.44089210e-16, 8.88178420e-16,\n",
-       "       1.55431223e-15, 2.66453526e-15, 3.99680289e-15, 5.55111512e-15,\n",
-       "       7.32747196e-15, 9.32587341e-15, 1.13242749e-14, 1.35447209e-14,\n",
-       "       1.62092562e-14, 1.90958360e-14, 2.22044605e-14, 2.55351296e-14,\n",
-       "       2.90878432e-14, 3.28626015e-14, 3.68594044e-14, 4.13002965e-14,\n",
-       "       4.59632332e-14, 5.08482145e-14, 5.59552404e-14, 6.12843110e-14,\n",
-       "       6.68354261e-14, 7.26085858e-14, 7.86037901e-14, 8.50430837e-14,\n",
-       "       9.17044218e-14, 9.85878046e-14, 1.05693232e-13, 1.13242749e-13,\n",
-       "       1.20792265e-13, 1.28563826e-13, 1.36779477e-13, 1.45217172e-13,\n",
-       "       1.53876911e-13, 1.62980740e-13, 1.72528658e-13, 1.81854531e-13,\n",
-       "       1.91624494e-13, 2.01838546e-13, 2.12274642e-13, 2.22932783e-13,\n",
-       "       2.33812969e-13, 2.45137244e-13, 2.56905608e-13, 2.68896017e-13,\n",
-       "       2.81108470e-13, 2.93765012e-13, 3.06643599e-13, 3.19744231e-13,\n",
-       "       3.33066907e-13, 3.46611628e-13, 3.60822483e-13, 3.75477427e-13,\n",
-       "       3.90132371e-13, 4.05231404e-13, 4.20774526e-13, 4.36761738e-13,\n",
-       "       4.52748949e-13, 4.69180250e-13, 4.86277685e-13, 5.03153075e-13,\n",
-       "       5.20472554e-13, 5.37792033e-13, 5.55999691e-13, 5.74651438e-13,\n",
-       "       5.93525229e-13, 6.12843110e-13, 6.32827124e-13, 6.52811138e-13,\n",
-       "       6.73017198e-13, 6.93223257e-13, 7.14317494e-13, 7.36077865e-13,\n",
-       "       7.57838237e-13, 7.79820652e-13, 8.02691247e-13, 8.25561841e-13,\n",
-       "...\n",
-       "       1.31983313e-11, 1.32187594e-11, 1.32370226e-11, 1.32530653e-11,\n",
-       "       1.32669986e-11, 1.32788225e-11, 1.32883704e-11, 1.32956424e-11,\n",
-       "       1.33005829e-11, 1.33031919e-11, 1.33035249e-11, 1.33012490e-11,\n",
-       "       1.32966971e-11, 1.32894806e-11, 1.32797107e-11, 1.32676092e-11,\n",
-       "       1.32526212e-11, 1.32353017e-11, 1.32149847e-11, 1.31921141e-11,\n",
-       "       1.31665789e-11, 1.31382683e-11, 1.31069600e-11, 1.30728761e-11,\n",
-       "       1.30360167e-11, 1.29962707e-11, 1.29535271e-11, 1.29078970e-11,\n",
-       "       1.28593802e-11, 1.28074218e-11, 1.27525768e-11, 1.26949562e-11,\n",
-       "       1.26338939e-11, 1.25698341e-11, 1.25023325e-11, 1.24318333e-11,\n",
-       "       1.23581145e-11, 1.22810651e-11, 1.22007959e-11, 1.21171961e-11,\n",
-       "       1.20300436e-11, 1.19397825e-11, 1.18460797e-11, 1.17490462e-11,\n",
-       "       1.16484600e-11, 1.15446541e-11, 1.14370735e-11, 1.13261622e-11,\n",
-       "       1.12119203e-11, 1.10941256e-11, 1.09725562e-11, 1.08476561e-11,\n",
-       "       1.07189813e-11, 1.05870868e-11, 1.04514175e-11, 1.03119735e-11,\n",
-       "       1.01691988e-11, 1.00233155e-11, 9.87299131e-12, 9.71933645e-12,\n",
-       "       9.56190682e-12, 9.40092448e-12, 9.23616739e-12, 9.06807962e-12,\n",
-       "       8.89599505e-12, 8.72013572e-12, 8.54050164e-12, 8.35753688e-12,\n",
-       "       8.17101942e-12, 7.98094923e-12, 7.78666021e-12, 7.58904051e-12,\n",
-       "       7.38742401e-12, 7.18247684e-12, 6.97397695e-12, 6.76170231e-12,\n",
-       "       6.54609700e-12, 6.32649488e-12])</pre></div></div></li><li class='xr-section-item'><input id='section-c8e83ee1-6210-4df1-b575-4f9572208741' class='xr-section-summary-in' type='checkbox'  checked><label for='section-c8e83ee1-6210-4df1-b575-4f9572208741' class='xr-section-summary' >Coordinates: <span>(2)</span></label><div class='xr-section-inline-details'></div><div class='xr-section-details'><ul class='xr-var-list'><li class='xr-var-item'><div class='xr-var-name'><span>id</span></div><div class='xr-var-dims'>()</div><div class='xr-var-dtype'>int64</div><div class='xr-var-preview xr-preview'>4</div><input id='attrs-63cb2379-a981-4348-833a-cbd1fede10c9' class='xr-var-attrs-in' type='checkbox' disabled><label for='attrs-63cb2379-a981-4348-833a-cbd1fede10c9' title='Show/Hide attributes'><svg class='icon xr-icon-file-text2'><use xlink:href='#icon-file-text2'></use></svg></label><input id='data-1826038b-6841-492f-bc15-44da3de4b3b6' class='xr-var-data-in' type='checkbox'><label for='data-1826038b-6841-492f-bc15-44da3de4b3b6' title='Show/Hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-var-attrs'><dl class='xr-attrs'></dl></div><div class='xr-var-data'><pre>array(4)</pre></div></li><li class='xr-var-item'><div class='xr-var-name'><span class='xr-has-index'>time (d)</span></div><div class='xr-var-dims'>(time (d))</div><div class='xr-var-dtype'>float64</div><div class='xr-var-preview xr-preview'>0.0 1.0 2.0 ... 363.0 364.0 365.0</div><input id='attrs-39689f27-9bf8-408c-b0b5-1b1b2e8cbbfd' class='xr-var-attrs-in' type='checkbox' disabled><label for='attrs-39689f27-9bf8-408c-b0b5-1b1b2e8cbbfd' title='Show/Hide attributes'><svg class='icon xr-icon-file-text2'><use xlink:href='#icon-file-text2'></use></svg></label><input id='data-5d1d9aad-0c7f-4cff-92aa-3f0374ee6a2c' class='xr-var-data-in' type='checkbox'><label for='data-5d1d9aad-0c7f-4cff-92aa-3f0374ee6a2c' title='Show/Hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-var-attrs'><dl class='xr-attrs'></dl></div><div class='xr-var-data'><pre>array([  0.,   1.,   2., ..., 363., 364., 365.])</pre></div></li></ul></div></li><li class='xr-section-item'><input id='section-58ebc301-6beb-4f02-92dc-c8dda8008e82' class='xr-section-summary-in' type='checkbox' disabled ><label for='section-58ebc301-6beb-4f02-92dc-c8dda8008e82' class='xr-section-summary'  title='Expand/collapse section'>Attributes: <span>(0)</span></label><div class='xr-section-inline-details'></div><div class='xr-section-details'><dl class='xr-attrs'></dl></div></li></ul></div></div>"
+       "  * time (d)  (time (d)) float64 0.0 1.0 2.0 3.0 4.0 ... 363.0 364.0 365.0 366.0</pre><div class='xr-wrap' hidden><div class='xr-header'><div class='xr-obj-type'>xarray.DataArray</div><div class='xr-array-name'>'px'</div><ul class='xr-dim-list'><li><span class='xr-has-index'>time (d)</span>: 367</li></ul></div><ul class='xr-sections'><li class='xr-section-item'><div class='xr-array-wrap'><input id='section-fabb7d40-273a-4c06-a3fc-0399e88877ca' class='xr-array-in' type='checkbox' checked><label for='section-fabb7d40-273a-4c06-a3fc-0399e88877ca' title='Show/hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-array-preview xr-preview'><span>0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0</span></div><div class='xr-array-data'><pre>array([0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.,\n",
+       "       0., 0., 0., 0., 0., 0., 0., 0., 0., 0.])</pre></div></div></li><li class='xr-section-item'><input id='section-de68d490-2721-4b5c-8b82-64e977e11680' class='xr-section-summary-in' type='checkbox'  checked><label for='section-de68d490-2721-4b5c-8b82-64e977e11680' class='xr-section-summary' >Coordinates: <span>(2)</span></label><div class='xr-section-inline-details'></div><div class='xr-section-details'><ul class='xr-var-list'><li class='xr-var-item'><div class='xr-var-name'><span>id</span></div><div class='xr-var-dims'>()</div><div class='xr-var-dtype'>int64</div><div class='xr-var-preview xr-preview'>4</div><input id='attrs-a358bd0d-ddc2-4083-90e7-b7cc9c5b89b4' class='xr-var-attrs-in' type='checkbox' disabled><label for='attrs-a358bd0d-ddc2-4083-90e7-b7cc9c5b89b4' title='Show/Hide attributes'><svg class='icon xr-icon-file-text2'><use xlink:href='#icon-file-text2'></use></svg></label><input id='data-f7240ece-94ad-45ca-aa8a-2a52ac1d28df' class='xr-var-data-in' type='checkbox'><label for='data-f7240ece-94ad-45ca-aa8a-2a52ac1d28df' title='Show/Hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-var-attrs'><dl class='xr-attrs'></dl></div><div class='xr-var-data'><pre>array(4)</pre></div></li><li class='xr-var-item'><div class='xr-var-name'><span class='xr-has-index'>time (d)</span></div><div class='xr-var-dims'>(time (d))</div><div class='xr-var-dtype'>float64</div><div class='xr-var-preview xr-preview'>0.0 1.0 2.0 ... 364.0 365.0 366.0</div><input id='attrs-4ce9e8f0-d411-4f33-9c83-325186b030b4' class='xr-var-attrs-in' type='checkbox' disabled><label for='attrs-4ce9e8f0-d411-4f33-9c83-325186b030b4' title='Show/Hide attributes'><svg class='icon xr-icon-file-text2'><use xlink:href='#icon-file-text2'></use></svg></label><input id='data-237faf6f-1ced-40e0-a252-a3faef7506b9' class='xr-var-data-in' type='checkbox'><label for='data-237faf6f-1ced-40e0-a252-a3faef7506b9' title='Show/Hide data repr'><svg class='icon xr-icon-database'><use xlink:href='#icon-database'></use></svg></label><div class='xr-var-attrs'><dl class='xr-attrs'></dl></div><div class='xr-var-data'><pre>array([  0.,   1.,   2., ..., 364., 365., 366.])</pre></div></li></ul></div></li><li class='xr-section-item'><input id='section-7f04a3a0-ecf9-4ee8-9c70-d473a2749c7f' class='xr-section-summary-in' type='checkbox' disabled ><label for='section-7f04a3a0-ecf9-4ee8-9c70-d473a2749c7f' class='xr-section-summary'  title='Expand/collapse section'>Attributes: <span>(0)</span></label><div class='xr-section-inline-details'></div><div class='xr-section-details'><dl class='xr-attrs'></dl></div></li></ul></div></div>"
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-       "...\n",
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        "Coordinates:\n",
        "    id        int64 4\n",
-       "  * time (d)  (time (d)) float64 0.0 1.0 2.0 3.0 4.0 ... 362.0 363.0 364.0 365.0"
+       "  * time (d)  (time (d)) float64 0.0 1.0 2.0 3.0 4.0 ... 363.0 364.0 365.0 366.0"
       ]
      },
      "execution_count": 8,
@@ -601,7 +550,7 @@
    "outputs": [
     {
      "data": {
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\n",
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\n",
       "text/plain": [
        "<Figure size 432x288 with 1 Axes>"
       ]
@@ -627,7 +576,7 @@
    "outputs": [
     {
      "data": {
-      "image/png": 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\n",
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\n",
       "text/plain": [
        "<Figure size 432x288 with 1 Axes>"
       ]
@@ -660,7 +609,7 @@
     },
     {
      "data": {
-      "image/png": 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\n",
+      "image/png": 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\n",
       "text/plain": [
        "<Figure size 432x288 with 1 Axes>"
       ]
@@ -695,7 +644,7 @@
     },
     {
      "data": {
-      "image/png": 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\n",
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\n",
       "text/plain": [
        "<Figure size 432x288 with 1 Axes>"
       ]
@@ -726,9 +675,9 @@
  ],
  "metadata": {
   "kernelspec": {
-   "display_name": "Python 3",
+   "display_name": "swiftestOOF",
    "language": "python",
-   "name": "python3"
+   "name": "swiftestoof"
   },
   "language_info": {
    "codemirror_mode": {
@@ -740,7 +689,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.8.6"
+   "version": "3.7.10"
   }
  },
  "nbformat": 4,
diff --git a/src/discard/discard.f90 b/src/discard/discard.f90
index 513a59122..daee4b15a 100644
--- a/src/discard/discard.f90
+++ b/src/discard/discard.f90
@@ -9,37 +9,35 @@ module subroutine discard_system(self, param)
       !! Adapted from David E. Kaufmann's Swifter routine: discard.f90
       !! Adapted from Hal Levison's Swift routine discard.f
       implicit none
-      class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-      class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters
+      class(swiftest_nbody_system), intent(inout) :: self    !! Swiftest system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters
 
       if (self%tp%nbody == 0) return 
-      select type(self)
+      select type(system => self)
       class is (whm_nbody_system)
-         associate(cb => self%cb, pl => self%pl, tp => self%tp, t => param%t, dt => param%dt, &
-                   msys => self%msys, discards => self%tp_discards, &
-                   ntp => self%tp%nbody, ldiscard => self%tp%ldiscard)
+         associate(cb => system%cb, pl => system%pl, npl => system%pl%nbody, tp => system%tp, ntp => system%tp%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
-                  call pl%h2b(cb) 
+                  if (npl > 0) call pl%h2b(cb) 
                   if (ntp > 0) call tp%h2b(cb) 
             end if
             if ((param%rmin >= 0.0_DP) .or. (param%rmax >= 0.0_DP) .or.  (param%rmaxu >= 0.0_DP)) then
-               if (ntp > 0) call tp%discard_sun(cb, param, t, msys)
+               if (ntp > 0) call tp%discard_sun(system, param)
             end if
-            if (param%qmin >= 0.0_DP .and. ntp > 0) call tp%discard_peri(cb, pl, param, t, msys)
-            if (param%lclose .and. ntp > 0) call tp%discard_pl(pl, t, dt)
+            if (param%qmin >= 0.0_DP .and. ntp > 0) call tp%discard_peri(system, param)
+            if (param%lclose .and. ntp > 0) call tp%discard_pl(system, param)
           
             if (any(tp%ldiscard(1:ntp))) then
                ! Spill the discards to the spill list
-               call tp%spill(discards, ldiscard)
-               call self%write_discard(param, discards)
+               call tp%spill(system%tp_discards, tp%ldiscard)
+               call self%write_discard(param, system%tp_discards)
             end if
          end associate  
          end select
       return
    end subroutine discard_system
 
-   module subroutine discard_sun_tp(self, cb, param, t, msys)
+   module subroutine discard_sun_tp(self, system, param)
       !! author: David A. Minton
       !!
       !!  Check to see if test particles should be discarded based on their positions relative to the Sun
@@ -49,16 +47,14 @@ module subroutine discard_sun_tp(self, cb, param, t, msys)
       !! Adapted from Hal Levison's Swift routine discard_sun.f
       implicit none
       ! Arguments
-      class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body object
-      class(swiftest_parameters), intent(in)    :: param !!  parameters parameters
-      real(DP),                      intent(in)    :: t      !! Current simulation tim
-      real(DP),                      intent(in)    :: msys   !! Total system mass
+      class(swiftest_tp),           intent(inout) :: self   !! Swiftest 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
       integer(I4B)        :: i
       real(DP)            :: energy, vb2, rb2, rh2, rmin2, rmax2, rmaxu2
 
-      associate(tp => self, ntp => self%nbody)
+      associate(tp => self, ntp => self%nbody, cb => system%cb, t => param%t, msys => system%msys)
          rmin2 = max(param%rmin * param%rmin, cb%radius * cb%radius)
          rmax2 = param%rmax**2
          rmaxu2 = param%rmaxu**2
@@ -90,7 +86,7 @@ module subroutine discard_sun_tp(self, cb, param, t, msys)
       return
    end subroutine discard_sun_tp
 
-   module subroutine discard_peri_tp(self, cb, pl, param, t, msys)
+   module subroutine discard_peri_tp(self, system, param)
       !! author: David A. Minton
       !!
       !! Check to see if a test particle should be discarded because its perihelion distance becomes too small
@@ -99,19 +95,16 @@ module subroutine discard_peri_tp(self, cb, pl, param, t, msys)
       !! Adapted from Hal Levison's Swift routine discard_peri.f
       implicit none
       ! Arguments
-      class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body object
-      class(swiftest_pl),            intent(inout) :: pl     !! Swiftest massive body object
-      class(swiftest_parameters), intent(in)    :: param !!  parameters parameters
-      real(DP),                      intent(in)    :: t      !! Current simulation tim
-      real(DP),                      intent(in)    :: msys   !! Total system mass 
+      class(swiftest_tp),           intent(inout) :: self   !! Swiftest test particle object
+      class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameterss
       ! Internals
       logical, save             :: lfirst = .true.
       integer(I4B)              :: i, j, ih
       real(DP)                  :: r2
       real(DP), dimension(NDIM) :: dx
    
-      associate(tp => self, ntp => self%nbody, npl => pl%nbody, qmin_coord => param%qmin_coord)
+      associate(cb => system%cb, tp => self, ntp => self%nbody, pl => system%pl, npl => system%pl%nbody, qmin_coord => param%qmin_coord, t => param%t, msys => system%msys)
          if (lfirst) then
             call util_hills(npl, pl)
             call util_peri(lfirst, ntp, tp, cb%Gmass, msys, param%qmin_coord)
@@ -145,7 +138,7 @@ module subroutine discard_peri_tp(self, cb, pl, param, t, msys)
    
    end subroutine discard_peri_tp
 
-   module subroutine discard_pl_tp(self, pl, t, dt)
+   module subroutine discard_pl_tp(self, system, param)
       !! author: David A. Minton
       !!
       !! Check to see if test particles should be discarded based on their positions relative to the massive bodies
@@ -154,16 +147,15 @@ module subroutine discard_pl_tp(self, pl, t, dt)
       !! Adapted from Hal Levison's Swift routine discard_pl.f
       implicit none
       ! Arguments
-      class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-      class(swiftest_pl),            intent(inout) :: pl     !! Swiftest massive body object
-      real(DP),                      intent(in)    :: t      !! Current simulation tim
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(swiftest_tp),           intent(inout) :: self   !! Swiftest 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 
       integer(I4B)              :: i, j, isp
       real(DP)                  :: r2min, radius
       real(DP), dimension(NDIM) :: dx, dv
    
-      associate(tp => self, ntp => self%nbody, npl => pl%nbody)
+      associate(tp => self, ntp => self%nbody, pl => system%pl, npl => system%pl%nbody, t => param%t, dt => param%dt)
          do i = 1, ntp
             if (tp%status(i) == ACTIVE) then
                do j = 1, npl
@@ -187,7 +179,7 @@ module subroutine discard_pl_tp(self, pl, t, dt)
    
    end subroutine discard_pl_tp
 
-   module subroutine discard_pl_close(dx, dv, dt, r2crit, iflag, r2min)
+   subroutine discard_pl_close(dx, dv, dt, r2crit, iflag, r2min)
       !! author: David A. Minton
       !!
       !!  Check to see if a test particle and massive body are having, or will have within the next time step, an encounter such
diff --git a/src/driftkick/drift.f90 b/src/drift/drift.f90
similarity index 100%
rename from src/driftkick/drift.f90
rename to src/drift/drift.f90
diff --git a/src/gr/gr.f90 b/src/gr/gr.f90
index d50968ad1..6afc9f5ed 100644
--- a/src/gr/gr.f90
+++ b/src/gr/gr.f90
@@ -1,7 +1,8 @@
 submodule(swiftest_classes) s_gr
    use swiftest
 contains
-   module procedure gr_getaccb_ns_body
+   subroutine gr_getaccb_ns_body(self, cb, param, agr, agr0) 
+
       !! author: David A. Minton
       !!
       !! Add relativistic correction acceleration for non-symplectic integrators
@@ -9,7 +10,13 @@
       !!
       !! Adapted from David A. Minton's Swifter routine routine gr_getaccb_ns.f90
       implicit none
-
+      ! Arguments
+      class(swiftest_body),          intent(inout) :: self
+      class(swiftest_cb),            intent(inout) :: cb
+      class(swiftest_parameters), intent(in)    :: param
+      real(DP), dimension(:, :),     intent(inout) :: agr
+      real(DP), dimension(NDIM),     intent(out)   :: agr0
+      ! Internals
       real(DP), dimension(NDIM) :: xh, vh
       real(DP)                  :: rmag, rdotv, vmag2
       integer(I4B)              :: i
@@ -29,7 +36,6 @@
          agr0 =  0.0_DP
          select type(self)
          class is (swiftest_pl)
-            !do concurrent(i = 1:NDIM)
             do i = 1, NDIM
                agr0(i) = -sum(self%Gmass(1:n) * agr(1:n, i) / msun)
             end do
@@ -39,6 +45,6 @@
 
       return
 
-   end procedure gr_getaccb_ns_body
+      end subroutine gr_getaccb_ns_body
 
 end submodule s_gr
\ No newline at end of file
diff --git a/src/helio/helio_drift.f90 b/src/helio/helio_drift.f90
index ff0adc03a..59f828425 100644
--- a/src/helio/helio_drift.f90
+++ b/src/helio/helio_drift.f90
@@ -1,7 +1,8 @@
 submodule (helio_classes) s_helio_drift
    use swiftest
 contains
-   module subroutine helio_drift_pl(self, cb, param, dt)
+   module subroutine helio_drift_pl(self, system, param, dt)
+
       !! author: David A. Minton
       !!
       !! Loop through massive bodies and call Danby drift routine
@@ -11,22 +12,17 @@ module subroutine helio_drift_pl(self, cb, param, dt)
       !! Adapted from Hal Levison's Swift routine drift.f
       implicit none
       ! Arguments
-      class(helio_pl),               intent(inout) :: self   !! Helio test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Helio central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(helio_pl),              intent(inout) :: self   !! Helio massive body object
+      class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: dt     !! Stepsize)
       ! Internals
       integer(I4B) :: i !! Loop counter
       real(DP) :: rmag, vmag2, energy
       integer(I4B), dimension(:),allocatable :: iflag !! Vectorized error code flag
       real(DP), dimension(:), allocatable          :: dtp
 
-      associate(npl    => self%nbody, &
-         xh     => self%xh, &
-         vb     => self%vb, &
-         status => self%status,&
-         mu     => self%mu)
-
+      associate(pl => self, npl => self%nbody)
          if (npl == 0) return
 
          allocate(iflag(npl))
@@ -35,23 +31,23 @@ module subroutine helio_drift_pl(self, cb, param, dt)
 
          if (param%lgr) then
             do i = 1,npl
-               rmag = norm2(xh(:, i))
-               vmag2 = dot_product(vb(:, i),  vb(:, i))
-               energy = 0.5_DP * vmag2 - mu(i) / rmag
+               rmag = norm2(pl%xh(:, i))
+               vmag2 = dot_product(pl%vb(:, i),  pl%vb(:, i))
+               energy = 0.5_DP * vmag2 - pl%mu(i) / rmag
                dtp(i) = dt * (1.0_DP + 3 * param%inv_c2 * energy)
             end do
          else
             dtp(:) = dt
          end if 
 
-         call drift_one(mu(1:npl), xh(1,1:npl), xh(2,1:npl), xh(3,1:npl), &
-                                   vb(1,1:npl), vb(2,1:npl), vb(3,1:npl), &
-                                   dtp(1:npl), iflag(1:npl))
+         call drift_one(pl%mu(1:npl), pl%xh(1,1:npl), pl%xh(2,1:npl), pl%xh(3,1:npl), &
+                                      pl%vb(1,1:npl), pl%vb(2,1:npl), pl%vb(3,1:npl), &
+                                      dtp(1:npl), iflag(1:npl))
          if (any(iflag(1:npl) /= 0)) then
             do i = 1, npl
-               write(*, *) " Planet ", self%name(i), " is lost!!!!!!!!!!"
-               write(*, *) xh(:,i)
-               write(*, *) vb(:,i)
+               write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
+               write(*, *) pl%xh(:,i)
+               write(*, *) pl%vb(:,i)
                write(*, *) " stopping "
                call util_exit(FAILURE)
             end do
@@ -94,7 +90,7 @@ module subroutine helio_drift_linear_pl(self, cb, dt, pt)
    
    end subroutine helio_drift_linear_pl
 
-   module subroutine helio_drift_tp(self, cb, param, dt)
+   module subroutine helio_drift_tp(self, system, param, dt)
       !! author: David A. Minton
       !!
       !! Loop through test particles and call Danby drift routine
@@ -103,21 +99,17 @@ module subroutine helio_drift_tp(self, cb, param, dt)
       !! Adapted from Hal Levison's Swift routine drift_tp.f
       implicit none
       ! Arguments
-      class(helio_tp),               intent(inout) :: self   !! Helio test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Helio central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(helio_tp),              intent(inout) :: self   !! Helio test particle object
+      class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: dt     !! Stepsiz
       ! Internals
       integer(I4B) :: i !! Loop counter
       real(DP) :: rmag, vmag2, energy
       real(DP), dimension(:), allocatable          :: dtp
       integer(I4B), dimension(:),allocatable :: iflag !! Vectorized error code flag
    
-      associate(ntp    => self%nbody, &
-         xh     => self%xh, &
-         vh     => self%vh, &
-         status => self%status,&
-         mu     => self%mu)
+      associate(tp => self, ntp => self%nbody)
          if (ntp == 0) return
          allocate(iflag(ntp))
          allocate(dtp(ntp))
@@ -128,21 +120,21 @@ module subroutine helio_drift_tp(self, cb, param, dt)
 
          if (param%lgr) then
             do i = 1,ntp
-               rmag = norm2(xh(:, i))
-               vmag2 = dot_product(vh(:, i),  vh(:, i))
-               energy = 0.5_DP * vmag2 - mu(i) / rmag
+               rmag = norm2(tp%xh(:, i))
+               vmag2 = dot_product(tp%vh(:, i), tp%vh(:, i))
+               energy = 0.5_DP * vmag2 - tp%mu(i) / rmag
                dtp(i) = dt * (1.0_DP + 3 * param%inv_c2 * energy)
             end do
          else
             dtp(:) = dt
          end if 
-         call drift_one(mu(1:ntp), xh(1,1:ntp), xh(2,1:ntp), xh(3,1:ntp), &
-                                   vh(1,1:ntp), vh(2,1:ntp), vh(3,1:ntp), &
-                                   dtp(1:ntp), iflag(1:ntp))
+         call drift_one(tp%mu(1:ntp), tp%xh(1,1:ntp), tp%xh(2,1:ntp), tp%xh(3,1:ntp), &
+                                      tp%vh(1,1:ntp), tp%vh(2,1:ntp), tp%vh(3,1:ntp), &
+                                      dtp(1:ntp), iflag(1:ntp))
          if (any(iflag(1:ntp) /= 0)) then
-            status = DISCARDED_DRIFTERR
+            tp%status = DISCARDED_DRIFTERR
             do i = 1, ntp
-               if (iflag(i) /= 0) write(*, *) "Particle ", self%name(i), " lost due to error in Danby drift"
+               if (iflag(i) /= 0) write(*, *) "Particle ", tp%name(i), " lost due to error in Danby drift"
             end do
          end if
       end associate
diff --git a/src/helio/helio_getacch.f90 b/src/helio/helio_getacch.f90
index 14fd76b4a..af6ab9e4d 100644
--- a/src/helio/helio_getacch.f90
+++ b/src/helio/helio_getacch.f90
@@ -1,7 +1,7 @@
 submodule (helio_classes) s_helio_getacch
    use swiftest
 contains
-   module subroutine helio_getacch_pl(self, cb, param, t)
+   module subroutine helio_getacch_pl(self, system, param, t)
       !! author: David A. Minton
       !!
       !! Compute heliocentric accelerations of massive bodies
@@ -10,10 +10,10 @@ module subroutine helio_getacch_pl(self, cb, param, t)
       !! Adapted from Hal Levison's Swift routine helio_getacch.f
       implicit none
       ! Arguments
-      class(helio_pl),               intent(inout) :: self     !! Helio massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb       !! Swiftest central body particle data structure
-      class(swiftest_parameters), intent(in)    :: param   !! Input collection of 
-      real(DP),                      intent(in)    :: t        !! Current time
+      class(helio_pl),              intent(inout) :: self   !! Helio massive body particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: t      !! Current simulation time
       ! Internals
       logical, save                    :: lmalloc = .true.
       integer(I4B)                     :: i
@@ -21,22 +21,19 @@ module subroutine helio_getacch_pl(self, cb, param, t)
       real(DP), dimension(:), allocatable, save    :: irh
       real(DP), dimension(:, :), allocatable, save :: xh_loc, aobl
 
-      associate(npl => self%nbody)
-         !if (lflag) then
-            self%ahi(:,2:npl) = 0.0_DP
-            call helio_getacch_int_pl(self, t)
-         !end if
-         !if (param%loblatecb) call self%obl_acc(cb) TODO: Fix this
-         !else
-         self%ah(:,:) = self%ahi(:,:)
-         !end if
-         if (param%lextra_force) call self%user_getacch(cb, param, t)
+      associate(cb => system%cb, pl => self, npl => self%nbody)
+         pl%ahi(:,2:npl) = 0.0_DP
+         call helio_getacch_int_pl(pl, t)
+         pl%ah(:,:) = pl%ahi(:,:)
+         if (param%loblatecb) call pl%obl_acc(cb)
+         if (param%lextra_force) call pl%user_getacch(system, param, t)
+         if (param%lgr) call pl%gr_getacch(param)
       end associate
 
       return
       end subroutine helio_getacch_pl
 
-      module subroutine helio_getacch_tp(self, cb, pl, param, t, xh)
+      module subroutine helio_getacch_tp(self, system, param, t, xhp)
          !! author: David A. Minton
          !!
          !! Compute heliocentric accelerations of test particles
@@ -45,34 +42,32 @@ module subroutine helio_getacch_tp(self, cb, pl, param, t, xh)
          !! Adapted from Hal Levison's Swift routine helio_getacch_tp.f
          implicit none
          ! Arguments
-         class(helio_tp),               intent(inout) :: self   !! Helio test particle data structure
-         class(swiftest_cb),                 intent(inout) :: cb     !! Swiftest central body particle data structuree 
-         class(whm_pl),                 intent(inout) :: pl     !! WHM massive body particle data structure. 
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
+         class(helio_tp),              intent(inout) :: self   !! WHM test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: t      !! Current time
+         real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets at the current substep
          ! Internals
          logical, save                                :: lmalloc = .true.
          integer(I4B)                                 :: i
          real(DP)                                     :: r2, mu
          real(DP), dimension(:), allocatable, save    :: irh, irht
-         real(DP), dimension(:, :), allocatable, save :: aobl, xht, aoblt
       
-      ! executable code
-         associate(ntp => self%nbody, npl => pl%nbody)
-            !if (lflag) then
+         associate(tp => self, ntp => self%nbody, cb => system%cb, pl => system%pl, npl => system%pl%nbody)
+            select type(pl => system%pl)
+            class is (helio_pl)
                self%ahi(:,:) = 0.0_DP
-               call helio_getacch_int_tp(self, pl, t, xh)
-            !end if
-            !if (param%loblatecb) call self%obl_acc(cb) TODO: Fix this
-            self%ah(:,:) = self%ahi(:,:)
-            if (param%lextra_force) call self%user_getacch(cb, param, t)
-            if (param%lgr) call self%gr_getacch(cb, param)
+               call helio_getacch_int_tp(tp, pl, t, xhp)
+               tp%ah(:,:) = tp%ahi(:,:)
+               if (param%loblatecb) call tp%obl_acc(cb) 
+               if (param%lextra_force) call tp%user_getacch(system, param, t)
+               if (param%lgr) call tp%gr_getacch(param)
+            end select
          end associate
          return
       end subroutine helio_getacch_tp
 
-      module subroutine helio_getacch_int_pl(self, t)
+      subroutine helio_getacch_int_pl(pl, t)
          !! author: David A. Minton
          !!
          !! Compute direct cross term heliocentric accelerations of massive bodiese
@@ -81,23 +76,23 @@ module subroutine helio_getacch_int_pl(self, t)
          !! Adapted from Hal Levison's Swift routine getacch_ah3.f
          implicit none
          ! Arguments
-         class(helio_pl),               intent(inout) :: self     !! Helio massive body particle data structure
-         real(DP),                      intent(in)    :: t        !! Current time
+         class(helio_pl), intent(inout) :: pl     !! Helio massive body particle data structure
+         real(DP),        intent(in)    :: t        !! Current time
          ! Internals
          integer(I4B)              :: i, j
          real(DP)                  :: rji2, irij3, faci, facj
          real(DP), dimension(NDIM) :: dx
       
-         associate(npl => self%nbody)
+         associate(npl => pl%nbody)
             do i = 2, npl - 1
                do j = i + 1, npl
-                  dx(:) = self%xh(:,j) - self%xh(:,i)
+                  dx(:) = pl%xh(:,j) - pl%xh(:,i)
                   rji2 = dot_product(dx(:), dx(:))
                   irij3 = 1.0_DP / (rji2 * sqrt(rji2))
-                  faci = self%Gmass(i) * irij3
-                  facj = self%Gmass(j) * irij3
-                  self%ahi(:,i) = self%ahi(:,i) + facj * dx(:)
-                  self%ahi(:,i) = self%ahi(:,j) - faci * dx(:)
+                  faci = pl%Gmass(i) * irij3
+                  facj = pl%Gmass(j) * irij3
+                  pl%ahi(:,i) = pl%ahi(:,i) + facj * dx(:)
+                  pl%ahi(:,i) = pl%ahi(:,j) - faci * dx(:)
                end do
             end do
          end associate
@@ -105,7 +100,7 @@ module subroutine helio_getacch_int_pl(self, t)
          return
       end subroutine helio_getacch_int_pl
 
-      module subroutine helio_getacch_int_tp(self, pl, t, xh)
+      subroutine helio_getacch_int_tp(tp, pl, t, xhp)
          !! author: David A. Minton
          !!
          !! Compute direct cross term heliocentric accelerations of test particles
@@ -114,23 +109,23 @@ module subroutine helio_getacch_int_tp(self, pl, t, xh)
          !! Adapted from Hal Levison's Swift routine getacch_ah3_tp.f
          implicit none
          ! Arguments
-         class(helio_tp),               intent(inout) :: self     !! Helio test particle data structure
-         class(whm_pl),               intent(inout) :: pl       !! Helio massive body particle data structure
-         real(DP),                      intent(in)    :: t        !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
+         class(helio_tp),          intent(inout) :: tp     !! Helio test particle data structure
+         class(swiftest_pl),       intent(inout) :: pl       !! Helio massive body particle data structure
+         real(DP),                 intent(in)    :: t        !! Current time
+         real(DP), dimension(:,:), intent(in)    :: xhp     !! Heliocentric positions of planets
          ! Internals
          integer(I4B)              :: i, j
          real(DP)                  :: r2, fac
          real(DP), dimension(NDIM) :: dx
       
-         associate(ntp => self%nbody, npl => pl%nbody)
+         associate(ntp => tp%nbody, npl => pl%nbody)
             do i = 1, ntp
-            if (self%status(i) == ACTIVE) then
+            if (tp%status(i) == ACTIVE) then
                do j = 2, npl
-                  dx(:) = self%xh(:,i) - xh(:,j)
+                  dx(:) = tp%xh(:,i) - xhp(:,j)
                   r2 = dot_product(dx(:), dx(:))
                   fac = pl%Gmass(j) / (r2 * sqrt(r2))
-                  self%ahi(:,i) = self%ahi(:,i) - fac * dx(:)
+                  tp%ahi(:,i) = tp%ahi(:,i) - fac * dx(:)
                end do
             end if
             end do
diff --git a/src/helio/helio_step.f90 b/src/helio/helio_step.f90
index df92c58c1..53052fc9e 100644
--- a/src/helio/helio_step.f90
+++ b/src/helio/helio_step.f90
@@ -1,7 +1,7 @@
 submodule(helio_classes) s_helio_step
    use swiftest
 contains
-   module subroutine helio_step_system(self, param)
+   module subroutine helio_step_system(self, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step massive bodies and and active test particles ahead in heliocentric coordinates
@@ -10,31 +10,34 @@ module subroutine helio_step_system(self, param)
       !! Adapted from David E. Kaufmann's Swifter routine helio_step.f90
       implicit none
       ! Arguments
-      class(helio_nbody_system),     intent(inout) :: self    !! Helio nbody system object
-      class(swiftest_parameters), intent(in)    :: param  !! Input collection of on parameters 
+      class(helio_nbody_system),  intent(inout) :: self   !! Helio nbody 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
 
-      select type(cb => self%cb)
-      class is (helio_cb)
-      select type(pl => self%pl)
-      class is (helio_pl)
-      select type(tp => self%tp)
-      class is (helio_tp)
-      associate(ntp => tp%nbody, npl => pl%nbody, t => param%t, dt => param%dt)
-         call pl%set_rhill(cb)
-         call tp%set_beg_end(xbeg = pl%xh)
-         call pl%step(cb, param, t, dt)
-         if (ntp > 0) then
-            call tp%set_beg_end(xend = pl%xh)
-            call tp%step(cb, pl, param, t, dt)
-         end if
-      end associate
-      end select
-      end select
+      select type(system => self)
+      class is (helio_nbody_system)
+         select type(cb => self%cb)
+         class is (helio_cb)
+            select type(pl => self%pl)
+            class is (helio_pl)
+               select type(tp => self%tp)
+               class is (helio_tp)
+                  call pl%set_rhill(cb)
+                  call system%set_beg_end(xbeg = pl%xh)
+                  call pl%step(system, param, t, dt)
+                  if (tp%nbody > 0) then
+                     call system%set_beg_end(xend = pl%xh)
+                     call tp%step(system, param, t, dt)
+                  end if
+               end select
+            end select
+         end select
       end select
       return
    end subroutine helio_step_system 
 
-   module subroutine helio_step_pl(self, cb, param, t, dt)
+   module subroutine helio_step_pl(self, system, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step massive bodies ahead Democratic Heliocentric method
@@ -43,37 +46,40 @@ module subroutine helio_step_pl(self, cb, param, t, dt)
       !! Adapted from Hal Levison's Swift routine helio_step_pl.f
       implicit none
       ! Arguments
-      class(helio_pl),               intent(inout) :: self   !! WHM massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Helio central body particle data structure
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(helio_pl),              intent(inout) :: self   !! Helio massive body particle data structure
+      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     !! Stepsize
       ! Internals 
-      integer(I4B)     :: i,npl
+      integer(I4B)     :: i
       real(DP)         :: dth, msys
       real(DP), dimension(NDIM) :: ptbeg, ptend !! TODO: Incorporate these into the tp structure
       logical, save :: lfirst = .true.
-   
-      npl = self%nbody
-      dth = 0.5_DP * dt
-      if (lfirst) then
-         call self%vh2vb(cb)
-         lfirst = .false.
-      end if
-      call self%lindrift(cb, dth, ptbeg)
-      call self%getacch(cb, param, t)
-      call self%kickvb(dth)
-      call self%drift(cb, param, dt)
-      call self%getacch(cb, param, t + dt)
-      call self%kickvb(dth)
-      call self%lindrift(cb, dth, ptend)
-      call self%vb2vh(cb)
+  
+      associate(pl => self, cb => system%cb)
+         dth = 0.5_DP * dt
+         if (lfirst) then
+            call pl%vh2vb(cb)
+            lfirst = .false.
+         end if
+         call pl%lindrift(cb, dth, ptbeg)
+         call pl%getacch(system, param, t)
+         call pl%kickvb(dth)
+
+         call pl%drift(system, param, dt)
+         call pl%getacch(system, param, t + dt)
+         call pl%kickvb(dth)
+         call pl%lindrift(cb, dth, ptend)
+         call pl%vb2vh(cb)
+      end associate
    
       return
    
    end subroutine helio_step_pl
 
-   module subroutine helio_step_tp(self, cb, pl, param, t, dt)
+   module subroutine helio_step_tp(self, system, param, t, dt)
+
       !! author: David A. Minton
       !!
       !! Step active test particles ahead using Democratic Heliocentric method
@@ -82,32 +88,33 @@ module subroutine helio_step_tp(self, cb, pl, param, t, dt)
       !! Adapted from Hal Levison's Swift routine helio_step_tp.f
       implicit none
       ! Arguments
-      class(helio_tp),                 intent(inout) :: self !! Helio test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-      class(whm_pl),                 intent(inout) :: pl     !! WHM massive body data structure
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(helio_tp),              intent(inout) :: self    !! Helio test particle data structure
+      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
       ! Internals
       logical, save  :: lfirst = .true. !! Flag to indicate that this is the first call
       real(DP) :: dth   !! Half step size
-      real(DP) :: mu    !! Central mass term
    
-   ! executable code
-      dth = 0.5_DP * dt
-      mu = cb%Gmass
-      if (lfirst) then
-         call self%vh2vb(vbcb = -self%ptbeg)
-         lfirst = .false.
-      end if
-      call self%lindrift(dth, self%ptbeg)
-      call self%getacch(cb, pl, param, t, self%xbeg)
-      call self%kickvb(dth)
-      call self%drift(cb, param, dt)
-      call self%getacch(cb, pl, param, t + dt, self%xend)
-      call self%kickvb(dth)
-      call self%lindrift(dth, self%ptend)
-      call self%vb2vh(vbcb = -self%ptend)
+      select type(system)
+      class is (helio_nbody_system)
+         associate(tp => self, cb => system%cb, pl => system%pl, xbeg => system%xbeg, xend => system%xend)
+            dth = 0.5_DP * dt
+            if (lfirst) then
+               call tp%vh2vb(vbcb = -tp%ptbeg)
+               lfirst = .false.
+            end if
+            call tp%lindrift(dth, tp%ptbeg)
+            call tp%getacch(system, param, t, xbeg)
+            call tp%kickvb(dth)
+            call tp%drift(system, param, dt)
+            call tp%getacch(system, param, t + dt, xend)
+            call tp%kickvb(dth)
+            call tp%lindrift(dth, tp%ptend)
+            call tp%vb2vh(vbcb = -tp%ptend)
+         end associate
+      end select
    
       return
    
diff --git a/src/io/io.f90 b/src/io/io.f90
index 0b75066af..c1774f7ca 100644
--- a/src/io/io.f90
+++ b/src/io/io.f90
@@ -13,7 +13,7 @@ module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg)
       !! Adapted from Martin Duncan's Swift routine io_init_param.f
       implicit none
       ! Arguments
-      class(swiftest_parameters), intent(inout) :: self       !! Collection of  parameters parameters
+      class(swiftest_parameters), intent(inout) :: self       !! Collection of parameters
       integer, intent(in)                          :: unit       !! File unit number
       character(len=*), intent(in)                 :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
                                                                  !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
@@ -316,7 +316,7 @@ module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg)
       !! Adapted from Martin Duncan's Swift routine io_dump_param.f
       implicit none
       ! Arguments
-      class(swiftest_parameters),intent(in)     :: self         !! Collection of  parameters parameters
+      class(swiftest_parameters),intent(in)     :: self         !! Collection of parameters
       integer, intent(in)                          :: unit       !! File unit number
       character(len=*), intent(in)                 :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
                                                                !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
@@ -392,11 +392,13 @@ module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg)
       write(unit, Lfmt) "ENERGY",                   self%lenergy
       !write(unit, Lfmt) "YARKOVSKY", self%lyarkovsky
       !write(unit, Lfmt) "YORP", self%lyorp
+      iostat = 0
+      iomsg = "UDIO not implemented"
 
       return
    end subroutine io_param_writer
 
-   module subroutine io_dump_param(self, param_file_name, t, dt)
+   module subroutine io_dump_param(self, param_file_name)
       !! author: David A. Minton
       !!
       !! Dump integration parameters to file
@@ -405,14 +407,12 @@ module subroutine io_dump_param(self, param_file_name, t, dt)
       !! Adapted from Martin Duncan's Swift routine io_dump_param.f
       implicit none
       ! Arguments
-      class(swiftest_parameters),intent(in) :: self    !! Output collection of  parameters
-      character(len=*), intent(in)             :: param_file_name !! Parameter input file name (i.e. param.in)
-      real(DP),intent(in)                      :: t       !! Current simulation time
-      real(DP),intent(in)                      :: dt      !! Step size
+      class(swiftest_parameters),intent(in) :: self    !! Output collection of parameters
+      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
+      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
@@ -434,7 +434,7 @@ module subroutine io_dump_param(self, param_file_name, t, dt)
       return
    end subroutine io_dump_param
 
-   module subroutine io_dump_swiftest(self, param, t, dt, msg) 
+   module subroutine io_dump_swiftest(self, param, msg) 
       !! author: David A. Minton
       !!
       !! Dump massive body data to files
@@ -443,11 +443,9 @@ module subroutine io_dump_swiftest(self, param, t, dt, msg)
       !! Adapted from Hal Levison's Swift routine io_dump_pl.f and io_dump_tp.f
       implicit none
       ! Arguments
-      class(swiftest_base),          intent(inout) :: self   !! Swiftest base object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of  parameters parameters 
-      real(DP),                      intent(in)    :: t      !! Current simulation time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
-      character(*), optional,        intent(in)    :: msg  !! Message to display with dump operation
+      class(swiftest_base),       intent(inout) :: self   !! Swiftest base object
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters 
+      character(*), optional,     intent(in)    :: msg  !! Message to display with dump operation
       ! Internals
       integer(I4B)                   :: ierr    !! Error code
       integer(I4B),parameter         :: LUN = 7 !! Unit number for dump file
@@ -468,13 +466,13 @@ module subroutine io_dump_swiftest(self, param, t, dt, msg)
          write(*, *) "   Unable to open binary dump file " // dump_file_name
          call util_exit(FAILURE)
       end if
-      call self%write_frame(iu, param, t, dt)
+      call self%write_frame(iu, param)
       close(LUN)
 
       return
    end subroutine io_dump_swiftest
 
-   module subroutine io_dump_system(self, param, t, dt, msg)
+   module subroutine io_dump_system(self, param, msg)
       !! author: David A. Minton
       !!
       !! Dumps the state of the system to files in case the simulation is interrupted.
@@ -482,11 +480,9 @@ module subroutine io_dump_system(self, param, t, dt, msg)
       !! so that if a dump file gets corrupted during writing, the user can restart from the older one.
       implicit none
       ! Arguments
-      class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-      class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
-      real(DP),                      intent(in)    :: t       !! Current simulation time
-      real(DP),                      intent(in)    :: dt      !! Stepsize
-      character(*), optional,        intent(in)    :: msg  !! Message to display with dump operation
+      class(swiftest_nbody_system), intent(inout) :: self    !! Swiftest system object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters 
+      character(*), optional,       intent(in)    :: msg  !! Message to display with dump operation
       ! Internals
       class(swiftest_parameters), allocatable :: dump_param   !! Local parameters variable used to parameters change input file names 
                                                     !!    to dump file-specific values without changing the user-defined values
@@ -495,26 +491,25 @@ module subroutine io_dump_system(self, param, t, dt, msg)
       character(len=:), allocatable :: param_file_name
       real(DP) :: tfrac
      
-
       allocate(dump_param, source=param)
-      param_file_name = trim(adjustl(DUMP_PARAM_FILE(idx)))
+      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%out_stat = 'APPEND'
-      call dump_param%dump(param_file_name,t,dt)
+      call dump_param%dump(param_file_name)
 
-      call self%cb%dump(dump_param, t, dt)
-      if (self%pl%nbody > 0) call self%pl%dump(dump_param, t, dt)
-      if (self%tp%nbody > 0) call self%tp%dump(dump_param, t, dt)
+      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)
 
       idx = idx + 1
       if (idx > NDUMPFILES) idx = 1
 
       ! Print the status message (format code passed in from main driver)
-      tfrac = (t - param%t0) / (param%tstop - param%t0)
-      write(*,msg) t, tfrac, self%pl%nbody, self%tp%nbody
+      tfrac = (param%t - param%t0) / (param%tstop - param%t0)
+      write(*,msg) param%t, tfrac, self%pl%nbody, self%tp%nbody
 
       return
    end subroutine io_dump_system
@@ -522,13 +517,13 @@ end subroutine io_dump_system
    module function io_get_args(integrator, param_file_name) result(ierr)
       !! author: David A. Minton
       !!
-      !! Reads in the name of the parameters file. 
+      !! Reads in the name of the parameter file from command line arguments. 
       implicit none
       ! Arguments
       integer(I4B)                  :: integrator      !! Symbolic code of the requested integrator  
       character(len=:), allocatable :: param_file_name !! Name of the input parameters file
       ! Result
-      integer(I4B)                  :: ierr             !! I/O error cod
+      integer(I4B)                  :: ierr             !! I/O error code
       ! Internals
       character(len=STRMAX) :: arg1, arg2
       integer :: narg,ierr_arg1, ierr_arg2
@@ -579,7 +574,7 @@ module function io_get_args(integrator, param_file_name) result(ierr)
       if (ierr /= 0) call util_exit(USAGE) 
    end function io_get_args
 
-   module function io_get_token(buffer, ifirst, ilast, ierr) result(token)
+   function io_get_token(buffer, ifirst, ilast, ierr) result(token)
       !! author: David A. Minton
       !!
       !! Retrieves a character token from an input string. Here a token is defined as any set of contiguous non-blank characters not 
@@ -588,12 +583,12 @@ module function io_get_token(buffer, ifirst, ilast, ierr) result(token)
       !! Adapted from David E. Kaufmann's Swifter routine io_get_token.f90
       implicit none
       ! Arguments
-      character(len=*), intent(in)     :: buffer         !! Input string buffer
-      integer(I4B), intent(inout)      :: ifirst         !! Index of the buffer at which to start the search for a token
-      integer(I4B), intent(out)        :: ilast          !! Index of the buffer at the end of the returned token
-      integer(I4B), intent(out)        :: ierr           !! Error code
+      character(len=*), intent(in)    :: buffer         !! Input string buffer
+      integer(I4B),     intent(inout) :: ifirst         !! Index of the buffer at which to start the search for a token
+      integer(I4B),     intent(out)   :: ilast          !! Index of the buffer at the end of the returned token
+      integer(I4B),     intent(out)   :: ierr           !! Error code
       ! Result
-      character(len=:),allocatable     :: token          !! Returned token string
+      character(len=:), allocatable   :: token          !! Returned token string
       ! Internals
       integer(I4B) :: i,ilength
    
@@ -635,8 +630,8 @@ module subroutine io_read_body_in(self, param)
       !! Adapted from Martin Duncan's Swift routine swiftest_init_pl.f and swiftest_init_tp.f
       implicit none
       ! Arguments
-      class(swiftest_body),          intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(inout) :: param !! Input collection of  parameters parameters
+      class(swiftest_body),       intent(inout) :: self   !! Swiftest particle object
+      class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters
       ! Internals
       integer(I4B), parameter       :: LUN = 7              !! Unit number of input file
       integer(I4B)                  :: iu = LUN
@@ -699,7 +694,7 @@ module subroutine io_read_body_in(self, param)
          read(iu, iostat = ierr) nbody
          call self%setup(nbody)
          if (nbody > 0) then
-            call self%read_frame(iu, param, XV, t, ierr)
+            call self%read_frame(iu, param, XV, ierr)
             self%status(:) = ACTIVE
          end if
       case default
@@ -724,7 +719,7 @@ module subroutine io_read_cb_in(self, param)
       !! Adapted from Martin Duncan's Swift routine swiftest_init_pl.f
       implicit none
       ! Arguments
-      class(swiftest_cb),            intent(inout) :: self
+      class(swiftest_cb),         intent(inout) :: self
       class(swiftest_parameters), intent(inout) :: param
       ! Internals
       integer(I4B), parameter :: LUN = 7              !! Unit number of input file
@@ -755,7 +750,7 @@ module subroutine io_read_cb_in(self, param)
             
       else
          open(unit = iu, file = param%incbfile, status = 'old', form = 'UNFORMATTED', iostat = ierr)
-         call self%read_frame(iu, param, XV, t, ierr)
+         call self%read_frame(iu, param, XV, ierr)
       end if
       close(iu)
       if (ierr /=  0) then
@@ -776,7 +771,7 @@ module subroutine io_read_param_in(self, param_file_name)
       !! Adapted from Martin Duncan's Swift routine io_init_param.f
       implicit none
       ! Arguments
-      class(swiftest_parameters),intent(out) :: self             !! Input collection of  parameters parameters
+      class(swiftest_parameters),intent(out) :: self             !! Current run configuration parameters
       character(len=*), intent(in)              :: param_file_name !! Parameter input file name (i.e. param.in)
       ! Internals
       integer(I4B), parameter :: LUN = 7                 !! Unit number of input file
@@ -808,7 +803,7 @@ module subroutine io_read_param_in(self, param_file_name)
       return 
    end subroutine io_read_param_in
 
-   module function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, &
+   function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, &
          xh1, xh2, vh1, vh2, encounter_file, out_type) result(ierr)
       !! author: David A. Minton
       !!
@@ -818,10 +813,10 @@ module function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius
       !! 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
-      real(DP), dimension(NDIM), intent(out) :: xh1, xh2, vh1, vh2
-      character(*), intent(in)      :: encounter_file, out_type
+      integer(I4B),           intent(out) :: name1, name2
+      real(DP),               intent(out) :: t, mass1, mass2, radius1, radius2
+      real(DP), dimension(:), intent(out) :: xh1, xh2, vh1, vh2
+      character(*),           intent(in)  :: encounter_file, out_type
       ! Result
       integer(I4B)         :: ierr
       ! Internals
@@ -858,7 +853,7 @@ module function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius
       return
    end function io_read_encounter
 
-   module subroutine io_read_frame_body(self, iu, param, form, t, ierr)
+   module subroutine io_read_frame_body(self, iu, param, form, ierr)
       !! author: David A. Minton
       !!
       !! Reads a frame of output of either test particle or massive body data to the binary output file
@@ -868,12 +863,11 @@ module subroutine io_read_frame_body(self, iu, param, form, t, ierr)
       !! Adapted from Hal Levison's Swift routine io_read_frame.F
       implicit none
       ! Arguments
-      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  !! Input collection of  parameters parameters 
-      character(*),                  intent(in)    :: form    !! Input format code ("XV" or "EL")
-      real(DP),                      intent(out)   :: t       !! Simulation time
-      integer(I4B),                  intent(out)   :: ierr    !! Error code
+      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
 
       associate(n => self%nbody)
          read(iu, iostat = ierr) self%name(1:n)
@@ -921,7 +915,7 @@ module subroutine io_read_frame_body(self, iu, param, form, t, ierr)
       return
    end subroutine io_read_frame_body
 
-   module subroutine io_read_frame_cb(self, iu, param, form, t, ierr)
+   module subroutine io_read_frame_cb(self, iu, param, form, ierr)
       !! author: David A. Minton
       !!
       !! Reads a frame of output of central body data to the binary output file
@@ -930,12 +924,11 @@ module subroutine io_read_frame_cb(self, iu, param, form, t, ierr)
       !! Adapted from Hal Levison's Swift routine io_read_frame.F
       implicit none
       ! Arguments
-      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   !! Input collection of  parameters parameters 
-      character(*),                  intent(in)    :: form     !! Input format code ("XV" or "EL")
-      real(DP),                      intent(out)   :: t        !! Simulation time
-      integer(I4B),                  intent(out)   :: ierr     !! Error cod
+      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
 
       read(iu, iostat = ierr) self%Gmass
       self%mass = self%Gmass / param%GU
@@ -958,18 +951,17 @@ module subroutine io_read_frame_cb(self, iu, param, form, t, ierr)
       return
    end subroutine io_read_frame_cb
  
-   module subroutine io_read_frame_system(self, iu, param, form, t, ierr)
+   module subroutine io_read_frame_system(self, iu, param, form, 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_parameters), intent(inout) :: param !! Input collection of  parameters parameters 
-      character(*),                  intent(in)    :: form   !! Input format code ("XV" or "EL")
-      real(DP),                      intent(out)   :: t      !! Current simulation time
-      integer(I4B),                  intent(out)   :: ierr   !! Error code
+      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
       ! Internals
       logical, save             :: lfirst = .true.
 
@@ -983,21 +975,21 @@ module subroutine io_read_frame_system(self, iu, param, form, t, ierr)
             return
          end if
       end if
-      ierr = io_read_hdr(iu, t, self%pl%nbody, self%tp%nbody, param%out_form, param%out_type)
+      ierr = io_read_hdr(iu, param%t, self%pl%nbody, self%tp%nbody, param%out_form, param%out_type)
       if (ierr /= 0) then
          write(*, *) "Swiftest error:"
          write(*, *) "   Binary output file already exists or cannot be accessed"
          return
       end if
-      call self%cb%read_frame(iu, param, form, t, ierr)
+      call self%cb%read_frame(iu, param, form, ierr)
       if (ierr /= 0) return
-      call self%pl%read_frame(iu, param, form, t, ierr)
+      call self%pl%read_frame(iu, param, form, ierr)
       if (ierr /= 0) return
-      call self%tp%read_frame(iu, param, form, t, ierr)
+      call self%tp%read_frame(iu, param, form, ierr)
       return
    end subroutine io_read_frame_system
 
-   module function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr)
+   function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr)
       !! author: David A. Minton
       !!
       !! Read frame header from input binary files
@@ -1009,7 +1001,7 @@ module function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr)
       integer(I4B), intent(in)   :: iu
       integer(I4B), intent(out)  :: npl, ntp
       character(*), intent(out)  ::  out_form
-      real(DP), intent(out)   :: t
+      real(DP),     intent(out)  :: t
       character(*), intent(in)   :: out_type
       ! Result
       integer(I4B)      :: ierr
@@ -1041,8 +1033,8 @@ module subroutine io_read_initialize_system(self, param)
       !!
       implicit none
       ! Arguments
-      class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-      class(swiftest_parameters), intent(inout) :: param  !! Input collection of  parameters parameters
+      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)
@@ -1062,9 +1054,9 @@ module subroutine io_write_discard(self, param, discards)
       !! Adapted from Hal Levison's Swift routine io_discard_write.f
       implicit none
       ! Arguments
-      class(swiftest_nbody_system),  intent(inout) :: self     !! Swiftest system object
-      class(swiftest_parameters), intent(in)    :: param   !! Input collection of  parameters parameters 
-      class(swiftest_body),          intent(inout) :: discards !! Swiftest discard object 
+      class(swiftest_nbody_system), intent(inout) :: self     !! Swiftest system object
+      class(swiftest_parameters),   intent(in)    :: param   !! Current run configuration parameters 
+      class(swiftest_body),         intent(inout) :: discards !! Swiftest discard object 
       ! Internals
       integer(I4B), parameter   :: LUN = 40
       integer(I4B)          :: i, ierr
@@ -1135,7 +1127,7 @@ module subroutine io_write_discard(self, param, discards)
    end subroutine io_write_discard
 
    module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, radius2, &
-                                          xh1, xh2, vh1, vh2, encounter_file, out_type)
+                                 xh1, xh2, vh1, vh2, encounter_file, out_type)
       !! author: David A. Minton
       !!
       !! Write close encounter data to output binary files
@@ -1145,10 +1137,10 @@ module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, rad
       !! Adapted from Hal Levison's Swift routine io_write_encounter.f
       implicit none
       ! Arguments
-      integer(I4B), intent(in)     :: name1, name2
-      real(DP), intent(in)      :: t, mass1, mass2, radius1, radius2
-      real(DP), dimension(NDIM), intent(in) :: xh1, xh2, vh1, vh2
-      character(*), intent(in)     :: encounter_file, out_type
+      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) :: encounter_file, out_type
       ! Internals
       logical , save    :: lfirst = .true.
       integer(I4B), parameter :: lun = 30
@@ -1184,7 +1176,7 @@ module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, rad
 
    end subroutine io_write_encounter
 
-   module subroutine io_write_frame_body(self, iu, param, t, dt)
+   module subroutine io_write_frame_body(self, iu, param)
       !! author: David A. Minton
       !!
       !! Write a frame of output of either test particle or massive body data to the binary output file
@@ -1194,11 +1186,9 @@ module subroutine io_write_frame_body(self, iu, param, t, dt)
       !! Adapted from Hal Levison's Swift routine io_write_frame.F
       implicit none
       ! Arguments
-      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 !! Input collection of  parameters parameters 
-      real(DP),                      intent(in)    :: t      !! Current simulation time
-      real(DP),                      intent(in)    :: dt     !! Step size
+      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 
 
       associate(n => self%nbody)
          if (n == 0) return
@@ -1241,7 +1231,7 @@ module subroutine io_write_frame_body(self, iu, param, t, dt)
       return
    end subroutine io_write_frame_body
 
-   module subroutine io_write_frame_cb(self, iu, param, t, dt)
+   module subroutine io_write_frame_cb(self, iu, param)
       !! author: David A. Minton
       !!
       !! Write a frame of output of central body data to the binary output file
@@ -1250,11 +1240,9 @@ module subroutine io_write_frame_cb(self, iu, param, t, dt)
       !! Adapted from Hal Levison's Swift routine io_write_frame.F
       implicit none
       ! Arguments
-      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 !! Input collection of  parameters parameters 
-      real(DP),                      intent(in)    :: t      !! Current simulation time
-      real(DP),                      intent(in)    :: dt     !! Step size
+      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 
 
       write(iu) self%Gmass
       write(iu) self%radius
@@ -1276,7 +1264,7 @@ module subroutine io_write_frame_cb(self, iu, param, t, dt)
       return
    end subroutine io_write_frame_cb
 
-   module subroutine io_write_frame_system(self, iu, param, t, dt)
+   module subroutine io_write_frame_system(self, iu, 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
@@ -1286,18 +1274,16 @@ module subroutine io_write_frame_system(self, iu, param, t, dt)
       !! 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 !! Input collection of  parameters parameters 
-      real(DP),                      intent(in)    :: t      !! Current simulation time
-      real(DP),                      intent(in)    :: dt     !! Step size
+      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 
       ! Internals
-      logical, save                         :: lfirst = .true. !! Flag to determine if this is the first call of this method
-      integer(I4B)                          :: ierr            !! I/O error code
+      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
+      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
 
       allocate(cb, source = self%cb)
       allocate(pl, source = self%pl)
@@ -1329,7 +1315,7 @@ module subroutine io_write_frame_system(self, iu, param, t, dt)
             call util_exit(FAILURE)
          end if
       end if
-      call io_write_hdr(iu, t, pl%nbody, tp%nbody, param%out_form, param%out_type)
+      call io_write_hdr(iu, param%t, pl%nbody, tp%nbody, param%out_form, param%out_type)
 
       if (param%lgr) then
          associate(vh => pl%vh, vht => tp%vh)
@@ -1350,9 +1336,9 @@ module subroutine io_write_frame_system(self, iu, param, t, dt)
       end if
       
       ! Write out each data type frame
-      call cb%write_frame(iu, param, t, dt)
-      call pl%write_frame(iu, param, t, dt)
-      call tp%write_frame(iu, param, t, dt)
+      call cb%write_frame(iu, param)
+      call pl%write_frame(iu, param)
+      call tp%write_frame(iu, param)
 
       deallocate(cb, pl, tp)
 
@@ -1361,7 +1347,7 @@ module subroutine io_write_frame_system(self, iu, param, t, dt)
       return
    end subroutine io_write_frame_system
 
-   module subroutine io_write_hdr(iu, t, npl, ntp, out_form, out_type)
+   subroutine io_write_hdr(iu, 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
diff --git a/src/driftkick/kick.f90 b/src/kick/kick.f90
similarity index 100%
rename from src/driftkick/kick.f90
rename to src/kick/kick.f90
diff --git a/src/main/swiftest_driver.f90 b/src/main/swiftest_driver.f90
index 166dbe409..b2384757a 100644
--- a/src/main/swiftest_driver.f90
+++ b/src/main/swiftest_driver.f90
@@ -12,7 +12,7 @@ program swiftest_driver
    class(swiftest_nbody_system), allocatable  :: nbody_system     !! Polymorphic object containing the nbody system to be integrated
    type(swiftest_parameters)               :: param
    integer(I4B)                               :: integrator       !! Integrator type code (see swiftest_globals for symbolic names)
-   character(len=:),allocatable               :: param_file_name !! Name of the file containing user-defined parameters parameters
+   character(len=:),allocatable               :: param_file_name !! Name of the file containing user-defined parameters
    integer(I4B)                               :: ierr             !! I/O error code 
    logical                                    :: lfirst           !! Flag indicating that this is the first time through the main loop
    integer(I8B)                               :: iloop            !! Loop counter
@@ -48,7 +48,7 @@ program swiftest_driver
       iloop = 0
       iout = istep_out
       idump = istep_dump
-      if (istep_out > 0) call nbody_system%write_frame(iu, param, t, dt)
+      if (istep_out > 0) call nbody_system%write_frame(iu, param)
       !> Define the maximum number of threads
       nthreads = 1            ! In the *serial* case
       !$ nthreads = omp_get_max_threads() ! In the *parallel* case
@@ -60,10 +60,9 @@ program swiftest_driver
          ntp = nbody_system%tp%nbody
          npl = nbody_system%pl%nbody
          !> Step the system forward in time
-         call nbody_system%step(param)
+         call nbody_system%step(param, t, dt)
 
          t = t0 + iloop * dt
-         if (t > tstop) exit 
 
          !> Evaluate any discards or mergers
          call nbody_system%discard(param)
@@ -72,7 +71,7 @@ program swiftest_driver
          if (istep_out > 0) then
             iout = iout - 1
             if (iout == 0) then
-               call nbody_system%write_frame(iu, param, t, dt)
+               call nbody_system%write_frame(iu, param)
                iout = istep_out
             end if
          end if
@@ -81,10 +80,11 @@ program swiftest_driver
          if (istep_dump > 0) then
             idump = idump - 1
             if (idump == 0) then
-               call nbody_system%dump(param, t, dt, statusfmt)
+               call nbody_system%dump(param, statusfmt)
                idump = istep_dump
             end if
          end if
+         if (t > tstop) exit 
       end do
 
       !> Dump the final state of the system to file
diff --git a/src/modules/helio_classes.f90 b/src/modules/helio_classes.f90
index d7b2d2d8d..ad10018a2 100644
--- a/src/modules/helio_classes.f90
+++ b/src/modules/helio_classes.f90
@@ -38,7 +38,6 @@ module helio_classes
       procedure, public :: drift       => helio_drift_pl        !! Method for Danby drift in Democratic Heliocentric coordinates 
       procedure, public :: lindrift    => helio_drift_linear_pl !! Method for linear drift of massive bodies due to barycentric momentum of Sun
       procedure, public :: getacch     => helio_getacch_pl      !! Compute heliocentric accelerations of massive bodies
-      procedure, public :: getacch_int => helio_getacch_int_pl  !! Compute direct cross term heliocentric accelerations of planets
       procedure, public :: setup       => helio_setup_pl        !! Constructor method - Allocates space for number of particles
       procedure, public :: step        => helio_step_pl         !! Steps the body forward one stepsize
    end type helio_pl
@@ -58,14 +57,11 @@ module helio_classes
       procedure, public :: drift       => helio_drift_tp        !! Method for Danby drift in Democratic Heliocentric coordinates 
       procedure, public :: lindrift    => helio_drift_linear_tp !! Method for linear drift of massive bodies due to barycentric momentum of Sun
       procedure, public :: getacch     => helio_getacch_tp      !! Compute heliocentric accelerations of massive bodies
-      procedure, public :: getacch_int => helio_getacch_int_tp   !! Compute direct cross term heliocentric accelerations of test particles
       procedure, public :: setup       => helio_setup_tp        !! Constructor method - Allocates space for number of particles
       procedure, public :: step        => helio_step_tp             !! Steps the body forward one stepsize
    end type helio_tp
 
-
    interface
-
       module subroutine helio_coord_vb2vh_pl(self, cb)
          use swiftest_classes, only : swiftest_cb
          implicit none
@@ -92,22 +88,22 @@ module subroutine helio_coord_vh2vb_tp(self, vbcb)
          real(DP), dimension(:), intent(in)    :: vbcb !! Barycentric velocity of the central body
       end subroutine helio_coord_vh2vb_tp
    
-      module subroutine helio_drift_pl(self, cb, param, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine helio_drift_pl(self, system, param, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(helio_pl),               intent(inout) :: self   !! Helio massive body object
-         class(swiftest_cb),            intent(inout) :: cb     !! Helio central body object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of parameters parameters
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(helio_pl),              intent(inout) :: self   !! Helio massive body object
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: dt     !! Stepsize
       end subroutine helio_drift_pl
 
-      module subroutine helio_drift_tp(self, cb, param, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine helio_drift_tp(self, system, param, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(helio_tp),               intent(inout) :: self   !! Helio test particle object
-         class(swiftest_cb),            intent(inout) :: cb     !! Helio central body object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of parameters parameters
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(helio_tp),              intent(inout) :: self   !! Helio test particle object
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: dt     !! Stepsize
       end subroutine helio_drift_tp
    
       module subroutine helio_drift_linear_pl(self, cb, dt, pt)
@@ -126,42 +122,25 @@ module subroutine helio_drift_linear_tp(self, dt, pt)
          real(DP), dimension(:),      intent(in)    :: pt     !! negative barycentric velocity of the Sun
       end subroutine helio_drift_linear_tp
 
-      module subroutine helio_getacch_pl(self, cb, param, t)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine helio_getacch_pl(self, system, param, t)
+         use swiftest_classes, only : swiftest_parameters, swiftest_nbody_system
          implicit none
-         class(helio_pl),               intent(inout) :: self     !! Helio massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb       !! Swiftest central body particle data structure
-         class(swiftest_parameters), intent(in)    :: param   !! Input collection of parameters parameters
-         real(DP),                      intent(in)    :: t        !! Current time
+         class(helio_pl),              intent(inout) :: self   !! Helio massive body particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: t      !! Current simulation time
       end subroutine helio_getacch_pl
 
-      module subroutine helio_getacch_tp(self, cb, pl, param, t, xh)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
-         use whm_classes, only : whm_pl
+      module subroutine helio_getacch_tp(self, system, param, t, xhp)
+         use swiftest_classes, only : swiftest_parameters, swiftest_nbody_system
          implicit none
-         class(helio_tp),               intent(inout) :: self   !! Helio test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree 
-         class(whm_pl),                 intent(inout) :: pl     !! Swiftest massive body particle data structure. 
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of parameters parameters
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
+         class(helio_tp),              intent(inout) :: self   !! Helio test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters
+         real(DP),                     intent(in)    :: t      !! Current time
+         real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets
       end subroutine helio_getacch_tp
 
-      module subroutine helio_getacch_int_pl(self, t)
-         implicit none
-         class(helio_pl),               intent(inout) :: self     !! Helio massive body particle data structure
-         real(DP),                      intent(in)    :: t        !! Current time
-      end subroutine helio_getacch_int_pl
-
-      module subroutine helio_getacch_int_tp(self, pl, t, xh)
-         use whm_classes, only : whm_pl
-         implicit none
-         class(helio_tp),               intent(inout) :: self     !! Helio test particle data structure
-         class(whm_pl),               intent(inout) :: pl       !! WhM massive body particle data structure
-         real(DP),                      intent(in)    :: t        !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planet
-      end subroutine helio_getacch_int_tp
-
       module subroutine helio_setup_pl(self, n)
          implicit none
          class(helio_pl), intent(inout) :: self !! Helio massive body object
@@ -174,33 +153,33 @@ module subroutine helio_setup_tp(self,n)
          integer,         intent(in)    :: n    !! Number of test particles to allocate
       end subroutine helio_setup_tp
 
-      module subroutine helio_step_system(self, param)
+      module subroutine helio_step_system(self, param, t, dt)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(helio_nbody_system),     intent(inout) :: self    !! Helio nbody system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
+         class(helio_nbody_system),  intent(inout) :: self   !! Helio nbody 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 
       end subroutine helio_step_system
 
-      module subroutine helio_step_pl(self, cb, param, t, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine helio_step_pl(self, system, param, t, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(helio_pl),               intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(helio_pl),              intent(inout) :: self   !! Helio massive body particle data structure
+         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     !! Stepsize
       end subroutine helio_step_pl
 
-      module subroutine helio_step_tp(self, cb, pl, param, t, dt)
+      module subroutine helio_step_tp(self, system, param, t, dt)
          use swiftest_classes, only : swiftest_cb, swiftest_parameters
-         use whm_classes, only : whm_pl
          implicit none
-         class(helio_tp),               intent(inout) :: self !! Helio test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-         class(whm_pl),                 intent(inout) :: pl     !! WHM massive body data structure
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(helio_tp),              intent(inout) :: self   !! Helio test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(inout) :: param  !! Current run configuration parameters 
+         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 881185af1..8fc57cadf 100644
--- a/src/modules/rmvs_classes.f90
+++ b/src/modules/rmvs_classes.f90
@@ -21,12 +21,15 @@ module rmvs_classes
    !********************************************************************************************************************************
    type, public, extends(whm_nbody_system) :: rmvs_nbody_system
       !> In the RMVS integrator, only test particles are discarded
-      logical                                  :: lplanetocentric = .false.   !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
+      logical                               :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
+      real(DP)                              :: rts                        !! fraction of Hill's sphere radius to use as radius of encounter region
+      real(DP), dimension(:,:), allocatable :: vbeg                       !! Planet velocities at beginning ot step
    contains
       private
       !> Replace the abstract procedures with concrete ones
       procedure, public :: initialize    => rmvs_setup_system  !! Performs RMVS-specific initilization steps, like calculating the Jacobi masses
       procedure, public :: step          => rmvs_step_system
+      procedure, public :: set_beg_end   => rmvs_setup_set_beg_end  !! Sets the beginning and ending values of planet positions. Also adds the end velocity for RMVS
    end type rmvs_nbody_system
 
    type, private :: rmvs_interp
@@ -40,9 +43,9 @@ module rmvs_classes
    !*******************************************************************************************************************************
    !> RMVS central body particle class 
    type, public, extends(whm_cb) :: rmvs_cb
-      logical                                   :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of test particles used for close encounter calculations
-      type(rmvs_interp),           dimension(:), allocatable :: outer !! interpolated heliocentric central body position for outer encounters
-      type(rmvs_interp),           dimension(:), allocatable :: inner !! interpolated heliocentric central body position for inner encounters
+      type(rmvs_interp), dimension(:), allocatable :: outer !! interpolated heliocentric central body position for outer encounters
+      type(rmvs_interp), dimension(:), allocatable :: inner !! interpolated heliocentric central body position for inner encounters
+      logical                                      :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
    end type rmvs_cb
 
    !********************************************************************************************************************************
@@ -54,24 +57,22 @@ module rmvs_classes
       !! Note to developers: If you add componenets to this class, be sure to update methods and subroutines that traverse the
       !!    component list, such as rmvs_setup_tp and rmvs_spill_tp
       ! encounter steps)
-      logical                                   :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of test particles used for close encounter calculations
       logical,      dimension(:),   allocatable :: lperi  !! planetocentric pericenter passage flag (persistent for a full rmvs time step) over a full RMVS time step)
       integer(I4B), dimension(:),   allocatable :: plperP !! index of planet associated with pericenter distance peri (persistent over a full RMVS time step)
       integer(I4B), dimension(:),   allocatable :: plencP !! index of planet that test particle is encountering (not persistent for a full RMVS time step)
-      real(DP),     dimension(:,:), allocatable :: vbeg   !! Planet velocities at beginning ot step
 
       ! The following are used to correctly set the oblateness values of the acceleration during an inner encounter with a planet
-      type(rmvs_cb)                             :: cb_heliocentric     !! Copy of original central body object passed to close encounter (used for oblateness acceleration during planetocentric encoountters)
-      real(DP),     dimension(:,:), allocatable :: xheliocentric !! original heliocentric position (used for oblateness calculation during close encounters)
-      integer(I4B)                              :: index   !!  inner substep number within current set
-      integer(I4B)                              :: ipleP   !!  index value of encountering planet
+      type(rmvs_cb)                             :: cb_heliocentric !! Copy of original central body object passed to close encounter (used for oblateness acceleration during planetocentric encoountters)
+      real(DP),     dimension(:,:), allocatable :: xheliocentric   !! original heliocentric position (used for oblateness calculation during close encounters)
+      integer(I4B)                              :: index           !!  inner substep number within current set
+      integer(I4B)                              :: ipleP           !!  index value of encountering planet
+      logical                                   :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
    contains
       procedure, public :: discard_pl        => rmvs_discard_pl_tp
       procedure, public :: encounter_check   => rmvs_encounter_check_tp !! Checks if any test particles are undergoing a close encounter with a massive body
       procedure, public :: fill              => rmvs_fill_tp            !! "Fills" bodies from one object into another depending on the results of a mask (uses the MERGE intrinsic)
       procedure, public :: getacch           => rmvs_getacch_tp         !!  Calculates either the standard or modified version of the acceleration depending if the
                                                                         !! if the test particle is undergoing a close encounter or not
-      procedure, public :: set_beg_end       => rmvs_setup_set_beg_end  !! Sets the beginning and ending values of planet positions. Also adds the end velocity for RMVS
       procedure, public :: setup             => rmvs_setup_tp           !! Constructor method - Allocates space for number of particles
       procedure, public :: spill             => rmvs_spill_tp           !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic)
    end type rmvs_tp
@@ -80,80 +81,82 @@ module rmvs_classes
    !                                    rmvs_pl class definitions and method interfaces
    !*******************************************************************************************************************************
  
-
    !> RMVS massive body particle class
-   type, private, extends(whm_pl) :: rmvs_base_pl
-      logical                                                :: lplanetocentric = .false.   !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
-      integer(I4B),                dimension(:), allocatable :: nenc    !! number of test particles encountering planet this full rmvs time step
-      integer(I4B),                dimension(:), allocatable :: tpenc1P !! index of first test particle encountering planet
-      integer(I4B),                dimension(:), allocatable :: plind ! Connects the planetocentric indices back to the heliocentric planet list
-      type(rmvs_interp),           dimension(:), allocatable :: outer !! interpolated heliocentric central body position for outer encounters
-      type(rmvs_interp),           dimension(:), allocatable :: inner !! interpolated heliocentric central body position for inner encounters
+   type, private, extends(whm_pl) :: rmvs_pl
+      integer(I4B),            dimension(:), allocatable :: nenc    !! number of test particles encountering planet this full rmvs time step
+      integer(I4B),            dimension(:), allocatable :: tpenc1P !! index of first test particle encountering planet
+      integer(I4B),            dimension(:), allocatable :: plind ! Connects the planetocentric indices back to the heliocentric planet list
+      type(rmvs_interp),       dimension(:), allocatable :: outer !! interpolated heliocentric central body position for outer encounters
+      type(rmvs_interp),       dimension(:), allocatable :: inner !! interpolated heliocentric central body position for inner encounters
+      class(rmvs_nbody_system), dimension(:), allocatable :: planetocentric
+      logical                                            :: lplanetocentric = .false.  !! Flag that indicates that the object is a planetocentric set of masive bodies used for close encounter calculations
    contains
       procedure, public :: fill                => rmvs_fill_pl    !! "Fills" bodies from one object into another depending on the results of a mask (uses the MERGE intrinsic)
       procedure, public :: setup               => rmvs_setup_pl    !! Constructor method - Allocates space for number of particles
       procedure, public :: spill               => rmvs_spill_pl    !! "Spills" bodies from one object to another depending on the results of a mask (uses the PACK intrinsic)
-   end type rmvs_base_pl
-
-   type, public :: rmvs_encounter_system
-      class(rmvs_cb),      allocatable :: cb
-      class(rmvs_tp),      allocatable :: tp
-      class(rmvs_base_pl), allocatable :: pl
-   end type rmvs_encounter_system
-
-   type, public, extends(rmvs_base_pl) :: rmvs_pl
-      type(rmvs_encounter_system), dimension(:), allocatable :: planetocentric
-      !! Note to developers: If you add componenets to this class, be sure to update methods and subroutines that traverse the
-      !!    component list, such as rmvs_setup_pl and rmvs_spill_pl
    end type rmvs_pl
-   
+
    interface
-      module subroutine rmvs_discard_pl_tp(self, pl, t, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_pl, swiftest_parameters
+      module subroutine rmvs_discard_pl_tp(self, system, param)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(rmvs_tp),                intent(inout) :: self
-         class(swiftest_pl),            intent(inout) :: pl     !! WHM massive body particle data structure. 
-         real(DP),                      intent(in)    :: t      !! Current simulation time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(rmvs_tp),               intent(inout) :: self   !! RMVS test particle object
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters 
       end subroutine rmvs_discard_pl_tp
 
-      module subroutine rmvs_getacch_tp(self, cb, pl, param, t, xh)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
-         use whm_classes, only : whm_pl
+      module function rmvs_encounter_check_tp(self, system, dt) result(lencounter)
          implicit none
-         class(rmvs_tp),                intent(inout) :: self   !! RMVS test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree 
-         class(whm_pl),                 intent(inout) :: pl     !! WHM massive body particle data structure. 
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of  parameter
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
-      end subroutine rmvs_getacch_tp
+         class(rmvs_tp),           intent(inout) :: self       !! RMVS test particle object  
+         class(rmvs_nbody_system), intent(inout) :: system     !! RMVS nbody system object
+         real(DP),                 intent(in)    :: dt         !! step size
+         logical                                 :: lencounter !! Returns true if there is at least one close encounter      
+      end function rmvs_encounter_check_tp
 
-      module subroutine rmvs_setup_system(self, param)
-         use swiftest_classes, only : swiftest_parameters
+      module subroutine rmvs_fill_pl(self, inserts, lfill_list)
+         use swiftest_classes, only : swiftest_body
          implicit none
-         class(rmvs_nbody_system),      intent(inout) :: self    !! RMVS system object
-         class(swiftest_parameters), intent(inout) :: param  !! Input collection of  parameters parameters 
-      end subroutine rmvs_setup_system
+         class(rmvs_pl),        intent(inout) :: self       !! RMVS massive body object 
+         class(swiftest_body),  intent(inout) :: inserts    !! Inserted object 
+         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
+      end subroutine rmvs_fill_pl
+
+      module subroutine rmvs_fill_tp(self, inserts, lfill_list)
+         use swiftest_classes, only : swiftest_body
+         implicit none
+         class(rmvs_tp),        intent(inout) :: self        !! RMVS massive body object
+         class(swiftest_body),  intent(inout) :: inserts     !!  Inserted object 
+         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
+      end subroutine rmvs_fill_tp
+
+      module subroutine rmvs_getacch_tp(self, system, param, t, xhp)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
+         implicit none
+         class(rmvs_tp),               intent(inout) :: self   !! RMVS test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest central body particle data structuree 
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters
+         real(DP),                     intent(in)    :: t      !! Current time
+         real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets at current substep
+      end subroutine rmvs_getacch_tp
 
       module subroutine rmvs_setup_pl(self,n)
          implicit none
-         class(rmvs_base_pl), intent(inout) :: self !! RMVS test particle object
+         class(rmvs_pl), intent(inout) :: self !! RMVS test particle object
          integer,             intent(in)    :: n    !! Number of test particles to allocate
       end subroutine rmvs_setup_pl
 
       module subroutine rmvs_setup_set_beg_end(self, xbeg, xend, vbeg)
          implicit none
-         class(rmvs_tp),           intent(inout)          :: self !! RMVS test particle object
+         class(rmvs_nbody_system), intent(inout)          :: self !! RMVS nbody system object
          real(DP), dimension(:,:), intent(in),   optional :: xbeg, xend, vbeg
       end subroutine rmvs_setup_set_beg_end
 
-      module subroutine rmvs_step_system(self, param)
+      module subroutine rmvs_setup_system(self, param)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(rmvs_nbody_system),      intent(inout) :: self    !! RMVS nbody system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
-      end subroutine rmvs_step_system
+         class(rmvs_nbody_system),   intent(inout) :: self    !! RMVS system object
+         class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters 
+      end subroutine rmvs_setup_system
 
       module subroutine rmvs_setup_tp(self,n)
          implicit none
@@ -161,32 +164,14 @@ module subroutine rmvs_setup_tp(self,n)
          integer,        intent(in)      :: n    !! Number of test particles to allocate
       end subroutine rmvs_setup_tp
 
-      module function rmvs_encounter_check_tp(self, cb, pl, dt, rts) result(lencounter)
-         implicit none
-         class(rmvs_tp),       intent(inout) :: self        !! RMVS test particle object  
-         class(rmvs_cb),       intent(inout) :: cb          !! RMVS central body object  
-         class(rmvs_pl),       intent(inout) :: pl          !! RMVS massive body object  
-         real(DP),             intent(in)    :: dt          !! step size
-         real(DP),             intent(in)    :: rts         !! fraction of Hill's sphere radius to use as radius of encounter regio
-         logical                             :: lencounter  !! Returns true if there is at least one close encounter      
-      end function rmvs_encounter_check_tp
-
       module subroutine rmvs_spill_pl(self, discards, lspill_list)
          use swiftest_classes, only : swiftest_body
          implicit none
-         class(rmvs_base_pl),   intent(inout) :: self      !! RMVS massive body object
+         class(rmvs_pl),   intent(inout) :: self      !! RMVS massive body object
          class(swiftest_body),  intent(inout) :: discards    !! Discarded object 
-         logical, dimension(:), intent(in)   :: lspill_list !! Logical array of bodies to spill into the discards
+         logical, dimension(:), intent(in)    :: lspill_list !! Logical array of bodies to spill into the discards
       end subroutine rmvs_spill_pl
 
-      module subroutine rmvs_fill_pl(self, inserts, lfill_list)
-         use swiftest_classes, only : swiftest_body
-         implicit none
-         class(rmvs_base_pl),   intent(inout) :: self       !! RMVS massive body object 
-         class(swiftest_body),  intent(inout) :: inserts    !! Inserted object 
-         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
-      end subroutine rmvs_fill_pl
-
       module subroutine rmvs_spill_tp(self, discards, lspill_list)
          use swiftest_classes, only : swiftest_body
          implicit none
@@ -195,13 +180,15 @@ module subroutine rmvs_spill_tp(self, discards, lspill_list)
          logical, dimension(:), intent(in)    :: lspill_list !! Logical array of bodies to spill into the discards
       end subroutine rmvs_spill_tp
 
-      module subroutine rmvs_fill_tp(self, inserts, lfill_list)
-         use swiftest_classes, only : swiftest_body
+      module subroutine rmvs_step_system(self, param, t, dt)
+         use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(rmvs_tp),        intent(inout) :: self        !! RMVS massive body object
-         class(swiftest_body),  intent(inout) :: inserts     !!  Inserted object 
-         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
-      end subroutine rmvs_fill_tp
+         class(rmvs_nbody_system),   intent(inout) :: self    !! RMVS nbody 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
+      end subroutine rmvs_step_system
+
    end interface
 
 end module rmvs_classes
diff --git a/src/modules/swiftest_classes.f90 b/src/modules/swiftest_classes.f90
index 7be1b04b3..f7ed5beb2 100644
--- a/src/modules/swiftest_classes.f90
+++ b/src/modules/swiftest_classes.f90
@@ -5,13 +5,28 @@ module swiftest_classes
    !! Adapted from David E. Kaufmann's Swifter routine: module_swifter.f90
    use swiftest_globals
    implicit none
-   public
+   private
+   public :: discard_pl_tp, discard_sun_tp, discard_system
+   public :: drift_one
+   public :: eucl_dist_index_plpl, eucl_dist_index_pltp, eucl_irij3_plpl
+   public :: kick_vb_body, kick_vh_body
+   public :: io_dump_param, io_dump_swiftest, io_dump_system, io_get_args, io_param_reader, io_param_writer, io_read_body_in, &
+             io_read_cb_in, io_read_param_in, io_read_frame_body, io_read_frame_cb, io_read_frame_system, io_read_initialize_system, &
+             io_write_discard, io_write_encounter, io_write_frame_body, io_write_frame_cb, io_write_frame_system
+   public :: obl_acc_body
+   public :: orbel_el2xv_vec, orbel_xv2el_vec, orbel_scget, orbel_xv2aeq, orbel_xv2aqt
+   public :: setup_body, setup_construct_system, setup_pl, setup_set_ir3h, setup_set_msys, setup_set_mu_pl, setup_set_mu_tp, &
+             setup_set_rhill, setup_tp
+   public :: user_getacch_body
+   public :: util_coord_b2h_pl, util_coord_b2h_tp, util_coord_h2b_pl, util_coord_h2b_tp, util_copy_body, util_copy_cb, util_copy_pl, &
+             util_copy_tp, util_copy_system, util_fill_body, util_fill_pl, util_fill_tp, util_reverse_status, util_spill_body, &
+             util_spill_pl, util_spill_tp
 
    !********************************************************************************************************************************
    ! swiftest_parameters class definitions 
    !********************************************************************************************************************************
 
-   !> User defined parameters parameters that are read in from the parameters input file. 
+   !> User defined parameters that are read in from the parameters input file. 
    !>    Each paramter is initialized to a default values. 
    type, public :: swiftest_parameters
       integer(I4B)         :: integrator     = UNKNOWN_INTEGRATOR !! Symbolic name of the nbody integrator  used
@@ -62,10 +77,11 @@ module swiftest_classes
       logical :: lyarkovsky = .false.        !! Turn on Yarkovsky effect
       logical :: lyorp = .false.             !! Turn on YORP effect
    contains
-      procedure :: reader         => io_param_reader
-      procedure :: writer         => io_param_writer
-      procedure :: dump           => io_dump_param
-      procedure :: read_from_file => io_read_param_in
+      private
+      procedure, public :: reader         => io_param_reader
+      procedure, public :: writer         => io_param_writer
+      procedure, public :: dump           => io_dump_param
+      procedure, public :: read_from_file => io_read_param_in
       !TODO: Figure out if user-defined derived-type io can be made to work properly
       !generic   :: read(FORMATTED) => param_reader
       !generic   :: write(FORMATTED) => param_writer
@@ -141,10 +157,9 @@ module swiftest_classes
       !!    component list, such as setup_body and util_spill
    contains
       private
-      procedure(abstract_set_mu),  public, deferred :: set_mu
-      procedure(abstract_gr_getacch), public, deferred :: gr_getacch
+      procedure(abstract_set_mu),     public, deferred :: set_mu
+      procedure(abstract_step_body),  public, deferred :: step
       ! These are concrete because the implementation is the same for all types of particles
-      procedure, public :: gr_getaccb     => gr_getaccb_ns_body  !! Add relativistic correction acceleration for non-symplectic integrators
       procedure, public :: initialize     => io_read_body_in     !! Read in body initial conditions from a file
       procedure, public :: read_frame     => io_read_frame_body  !! I/O routine for writing out a single frame of time-series data for the central body
       procedure, public :: write_frame    => io_write_frame_body !! I/O routine for writing out a single frame of time-series data for the central body
@@ -268,92 +283,80 @@ subroutine abstract_copy(self, src, mask)
          logical, dimension(:),        intent(in)    :: mask
       end subroutine abstract_copy 
 
-      subroutine abstract_gr_getacch(self, cb, param)
-         import swiftest_body, swiftest_cb, swiftest_parameters
-         class(swiftest_body),          intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of  parameter
-      end subroutine abstract_gr_getacch
-
       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   !! Input collection of  parameters parameters 
+         class(swiftest_parameters), intent(inout) :: param   !! Current run configuration parameters 
       end subroutine abstract_initialize
 
-      subroutine abstract_read_frame(self, iu, param, form, t, ierr)
+      subroutine abstract_read_frame(self, iu, param, form, 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   !! Input collection of  parameters parameters 
+         class(swiftest_parameters), intent(inout) :: param   !! Current run configuration parameters 
          character(*),                  intent(in)    :: form     !! Input format code ("XV" or "EL")
-         real(DP),                      intent(out)   :: t        !! Simulation time
          integer(I4B),                  intent(out)   :: ierr     !! Error code
       end subroutine abstract_read_frame
 
       subroutine abstract_set_mu(self, cb) 
          import swiftest_body, swiftest_cb
          class(swiftest_body),         intent(inout) :: self !! Swiftest particle object
-         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body objectt
+         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body object
       end subroutine abstract_set_mu
 
-      subroutine abstract_step_system(self, param)
-         import swiftest_nbody_system, swiftest_parameters
+      subroutine abstract_step_body(self, system, param, t, dt)
+         import DP, swiftest_body, swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
+         class(swiftest_body),         intent(inout) :: self   !! Swiftest particle 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
+      end subroutine abstract_step_body
+
+      subroutine abstract_step_system(self, param, t, dt)
+         import DP, swiftest_nbody_system, swiftest_parameters
+         implicit none
+         class(swiftest_nbody_system), intent(inout) :: self   !! 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
       end subroutine abstract_step_system
 
-      subroutine abstract_write_frame(self, iu, param, t, dt)
+      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   !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t        !! Current simulation time
-         real(DP),                      intent(in)    :: dt       !! Step size
+         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
-      module subroutine discard_peri_tp(self, cb, pl, param, t, msys)
-         implicit none
-         class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body object
-         class(swiftest_pl),            intent(inout) :: pl     !! Swiftest massive body object
-         class(swiftest_parameters), intent(in)    :: param !!  parameters parameters
-         real(DP),                      intent(in)    :: t      !! Current simulation tim
-         real(DP),                      intent(in)    :: msys   !! Total system mass
-      end subroutine discard_peri_tp
-
-      module subroutine discard_pl_close(dx, dv, dt, r2crit, iflag, r2min)
+      module subroutine discard_peri_tp(self, system, param)
          implicit none
-         real(DP), dimension(:), intent(in)    :: dx, dv
-         real(DP), intent(in)                  :: dt, r2crit
-         integer(I4B), intent(out)             :: iflag
-         real(DP), intent(out)                 :: r2min
-      end subroutine discard_pl_close
+         class(swiftest_tp),           intent(inout) :: self   !! Swiftest test particle object
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameter
+      end subroutine discard_peri_tp
 
-      module subroutine discard_pl_tp(self, pl, t, dt)
+      module subroutine discard_pl_tp(self, system, param)
          implicit none
-         class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-         class(swiftest_pl),            intent(inout) :: pl     !! Swiftest massive body object
-         real(DP),                      intent(in)    :: t      !! Current simulation tim
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(swiftest_tp),           intent(inout) :: self   !! Swiftest test particle object
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameter
       end subroutine discard_pl_tp
 
-      module subroutine discard_sun_tp(self, cb, param, t, msys)
+      module subroutine discard_sun_tp(self, system, param)
          implicit none
-         class(swiftest_tp),            intent(inout) :: self   !! Swiftest test particle object
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body object
-         class(swiftest_parameters), intent(in)    :: param !!  parameters parameters
-         real(DP),                      intent(in)    :: t      !! Current simulation tim
-         real(DP),                      intent(in)    :: msys   !! Total system mass
+         class(swiftest_tp),           intent(inout) :: self   !! Swiftest test particle object
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters
       end subroutine discard_sun_tp
 
       module subroutine discard_system(self, param)
          implicit none
-         class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
+         class(swiftest_nbody_system), intent(inout) :: self    !! Swiftest system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters 
       end subroutine discard_system
 
       module pure elemental subroutine drift_one(mu, px, py, pz, vx, vy, vz, dt, iflag)
@@ -366,33 +369,24 @@ end subroutine drift_one
 
       module subroutine eucl_dist_index_plpl(self)
          implicit none
-         class(swiftest_pl),             intent(inout) :: self  !! Swiftest massive body object
+         class(swiftest_pl), intent(inout) :: self  !! Swiftest massive body object
       end subroutine
 
       module subroutine eucl_dist_index_pltp(self, pl)
          implicit none
-         class(swiftest_tp),             intent(inout) :: self  !! Swiftest test particle object
-         class(swiftest_pl),             intent(inout) :: pl    !! Swiftest massive body object
+         class(swiftest_tp), intent(inout) :: self  !! Swiftest test particle object
+         class(swiftest_pl), intent(inout) :: pl    !! Swiftest massive body object
       end subroutine
 
       module subroutine eucl_irij3_plpl(self)
          implicit none
-         class(swiftest_pl),             intent(inout) :: self  !! Swiftest massive body object
+         class(swiftest_pl), intent(inout) :: self  !! Swiftest massive body object
       end subroutine eucl_irij3_plpl
 
-      module subroutine gr_getaccb_ns_body(self, cb, param, agr, agr0) 
-         implicit none
-         class(swiftest_body),          intent(inout) :: self
-         class(swiftest_cb),            intent(inout) :: cb
-         class(swiftest_parameters), intent(in)    :: param
-         real(DP), dimension(:, :),     intent(inout) :: agr
-         real(DP), dimension(NDIM),     intent(out)   :: agr0
-      end subroutine gr_getaccb_ns_body
-
       module subroutine kick_vb_body(self, dt)
          implicit none
-         class(swiftest_body),         intent(inout) :: self !! Swiftest generic body object
-         real(DP),                     intent(in)    :: dt   !! Stepsize
+         class(swiftest_body), intent(inout) :: self !! Swiftest generic body object
+         real(DP),             intent(in)    :: dt   !! Stepsize
       end subroutine kick_vb_body
 
       module subroutine kick_vh_body(self, dt)
@@ -401,48 +395,23 @@ module subroutine kick_vh_body(self, dt)
          real(DP),                     intent(in)    :: dt   !! Stepsize
       end subroutine kick_vh_body
 
-      module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) 
-         class(swiftest_parameters), intent(inout) :: self       !! Collection of  parameters parameters
-         integer, intent(in)                          :: unit       !! File unit number
-         character(len=*), intent(in)                 :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
-                                                                  !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
-         integer, intent(in)                          :: v_list(:)  !! The first element passes the integrator code to the reader
-         integer, intent(out)                         :: iostat     !! IO status code
-         character(len=*), intent(inout)              :: iomsg      !! Message to pass if iostat /= 0
-      end subroutine io_param_reader
-
-      module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg) 
-         class(swiftest_parameters),intent(in)     :: self         !! Collection of  parameters parameters
-         integer, intent(in)                          :: unit       !! File unit number
-         character(len=*), intent(in)                 :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
-                                                                  !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
-         integer, intent(in)                          :: v_list(:)  !! Not used in this procedure
-         integer, intent(out)                         :: iostat     !! IO status code
-         character(len=*), intent(inout)              :: iomsg      !! Message to pass if iostat /= 0
-      end subroutine io_param_writer
-
-      module subroutine io_dump_param(self, param_file_name, t, dt)
-         class(swiftest_parameters),intent(in) :: self    !! Output collection of  parameters
-         character(len=*), intent(in)             :: param_file_name !! Parameter input file name (i.e. param.in)
-         real(DP),intent(in)                      :: t       !! Current simulation time
-         real(DP),intent(in)                      :: dt      !! Step size
+      module subroutine io_dump_param(self, param_file_name)
+         implicit none
+         class(swiftest_parameters),intent(in)    :: self    !! Output collection of parameters
+         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, t, dt, msg) 
+      module subroutine io_dump_swiftest(self, param, msg) 
          implicit none
          class(swiftest_base),          intent(inout) :: self   !! Swiftest base object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t      !! Current simulation time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(swiftest_parameters),    intent(in)    :: param !! Current run configuration parameters 
          character(*), optional,        intent(in)    :: msg  !! Message to display with dump operation
       end subroutine io_dump_swiftest
 
-      module subroutine io_dump_system(self, param, t, dt, msg)
+      module subroutine io_dump_system(self, param, msg)
          implicit none
          class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t       !! Current simulation time
-         real(DP),                      intent(in)    :: dt      !! Stepsize
+         class(swiftest_parameters),    intent(in)    :: param  !! Current run configuration parameters 
          character(*), optional,        intent(in)    :: msg  !! Message to display with dump operation
       end subroutine io_dump_system
 
@@ -450,142 +419,119 @@ module function io_get_args(integrator, param_file_name) result(ierr)
          implicit none
          integer(I4B)                  :: integrator      !! Symbolic code of the requested integrator  
          character(len=:), allocatable :: param_file_name !! Name of the input parameters file
-         integer(I4B)                  :: ierr             !! I/O error code
+         integer(I4B)                  :: ierr             !! I/O error code 
       end function io_get_args
 
-      module function io_get_token(buffer, ifirst, ilast, ierr) result(token)
-         character(len=*), intent(in)     :: buffer         !! Input string buffer
-         integer(I4B), intent(inout)      :: ifirst         !! Index of the buffer at which to start the search for a token
-         integer(I4B), intent(out)        :: ilast          !! Index of the buffer at the end of the returned token
-         integer(I4B), intent(out)        :: ierr           !! Error code
-         character(len=:),allocatable     :: token          !! Returned token string
-      end function io_get_token
+      module subroutine io_param_reader(self, unit, iotype, v_list, iostat, iomsg) 
+         implicit none
+         class(swiftest_parameters), intent(inout) :: self       !! Collection of parameters
+         integer(I4B),               intent(in)    :: unit       !! File unit number
+         character(len=*),           intent(in)    :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
+                                                                 !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
+         integer(I4B),               intent(in)    :: v_list(:)  !! The first element passes the integrator code to the reader
+         integer(I4B),               intent(out)   :: iostat     !! IO status code
+         character(len=*),           intent(inout) :: iomsg      !! Message to pass if iostat /= 0
+      end subroutine io_param_reader
+
+      module subroutine io_param_writer(self, unit, iotype, v_list, iostat, iomsg) 
+         implicit none
+         class(swiftest_parameters), intent(in)    :: self         !! Collection of parameters
+         integer(I4B),               intent(in)    :: unit       !! File unit number
+         character(len=*),           intent(in)    :: iotype     !! Dummy argument passed to the  input/output procedure contains the text from the char-literal-constant, prefixed with DT. 
+                                                                 !!    If you do not include a char-literal-constant, the iotype argument contains only DT.
+         integer(I4B),               intent(in)    :: v_list(:)  !! Not used in this procedure
+         integer(I4B),               intent(out)   :: iostat     !! IO status code
+         character(len=*),           intent(inout) :: iomsg      !! Message to pass if iostat /= 0
+      end subroutine io_param_writer
 
       module subroutine io_read_body_in(self, param) 
          implicit none
-         class(swiftest_body),          intent(inout) :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(inout) :: param !! Input collection of  parameters parameters
+         class(swiftest_body),       intent(inout) :: self   !! Swiftest particle object
+         class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters
       end subroutine io_read_body_in
 
       module subroutine io_read_cb_in(self, param) 
          implicit none
-         class(swiftest_cb),            intent(inout) :: self
+         class(swiftest_cb),         intent(inout) :: self
          class(swiftest_parameters), intent(inout) :: param
       end subroutine io_read_cb_in
 
       module subroutine io_read_param_in(self, param_file_name) 
-         class(swiftest_parameters),intent(out) :: self             !! Input collection of  parameters parameters
-         character(len=*), intent(in)              :: param_file_name !! Parameter input file name (i.e. param.in)
-      end subroutine io_read_param_in
-
-      module function io_read_encounter(t, name1, name2, mass1, mass2, radius1, radius2, &
-                                           xh1, xh2, vh1, vh2, encounter_file, out_type) result(ierr)
          implicit none
-         integer(I4B)         :: ierr
-         integer(I4B), intent(out)     :: name1, name2
-         real(DP), intent(out)      :: t, mass1, mass2, radius1, radius2
-         real(DP), dimension(NDIM), intent(out) :: xh1, xh2, vh1, vh2
-         character(*), intent(in)      :: encounter_file,out_type
-      end function io_read_encounter
+         class(swiftest_parameters), intent(out) :: 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
 
-      module subroutine io_read_frame_body(self, iu, param, form, t, ierr)
+      module subroutine io_read_frame_body(self, iu, param, form, ierr)
          implicit none
-         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  !! Input collection of  parameters parameters 
-         character(*),                  intent(in)    :: form    !! Input format code ("XV" or "EL")
-         real(DP),                      intent(out)   :: t       !! Simulation time
-         integer(I4B),                  intent(out)   :: ierr    !! Error code
+         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
       end subroutine io_read_frame_body
 
-      module subroutine io_read_frame_cb(self, iu, param, form, t, ierr)
+      module subroutine io_read_frame_cb(self, iu, param, form, 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   !! Input collection of  parameters parameters 
-         character(*),                  intent(in)    :: form     !! Input format code ("XV" or "EL")
-         real(DP),                      intent(out)   :: t        !! Simulation time
-         integer(I4B),                  intent(out)   :: ierr     !! Error code
+         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
 
-      module subroutine io_read_frame_system(self, iu, param, form, t, ierr)
+      module subroutine io_read_frame_system(self, iu, param, form, 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 !! Input collection of  parameters parameters 
-         character(*),                  intent(in)    :: form   !! Input format code ("XV" or "EL")
-         real(DP),                      intent(out)   :: t      !! Current simulation time
-         integer(I4B),                  intent(out)   :: ierr   !! Error code
+         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
 
-      module function io_read_hdr(iu, t, npl, ntp, out_form, out_type) result(ierr)
-         implicit none
-         integer(I4B)      :: ierr
-         integer(I4B), intent(in)   :: iu
-         integer(I4B), intent(out)  :: npl, ntp
-         character(*), intent(out)  ::  out_form
-         real(DP), intent(out)   :: t
-         character(*), intent(in)   :: out_type
-      end function io_read_hdr
-
       module subroutine io_read_initialize_system(self, param)
          implicit none
          class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system object
-         class(swiftest_parameters), intent(inout) :: param  !! Input collection of  parameters parameters 
+         class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters 
       end subroutine io_read_initialize_system
 
       module subroutine io_write_discard(self, param, discards)
          implicit none
          class(swiftest_nbody_system),  intent(inout) :: self     !! Swiftest system object
-         class(swiftest_parameters), intent(in)    :: param   !! Input collection of  parameters parameters 
+         class(swiftest_parameters), intent(in)    :: param   !! Current run configuration parameters 
          class(swiftest_body),          intent(inout) :: discards !! Swiftest discard object 
       end subroutine io_write_discard
 
       module subroutine io_write_encounter(t, name1, name2, mass1, mass2, radius1, radius2, &
-                                             xh1, xh2, vh1, vh2, encounter_file, out_type)
+                                           xh1, xh2, vh1, vh2, encounter_file, out_type)
          implicit none
-         integer(I4B), intent(in)     :: name1, name2
-         real(DP), intent(in)      :: t, mass1, mass2, radius1, radius2
-         real(DP), dimension(NDIM), intent(in) :: xh1, xh2, vh1, vh2
-         character(*), intent(in)     :: encounter_file, out_type
+         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) :: encounter_file, out_type
       end subroutine io_write_encounter
 
-      module subroutine io_write_frame_body(self, iu, param, t, dt)
+      module subroutine io_write_frame_body(self, iu, param)
          implicit none
-         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 !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t      !! Current simulation time
-         real(DP),                      intent(in)    :: dt     !! Step size
+         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 
       end subroutine io_write_frame_body
 
-      module subroutine io_write_frame_cb(self, iu, param, t, dt)
+      module subroutine io_write_frame_cb(self, iu, param)
          implicit none
-         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 !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t      !! Current simulation time
-         real(DP),                      intent(in)    :: dt     !! Step size
+         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 
       end subroutine io_write_frame_cb
 
-      module subroutine io_write_frame_system(self, iu, param, t, dt)
+      module subroutine io_write_frame_system(self, iu, param)
          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 !! Input collection of  parameters parameters 
-         real(DP),                      intent(in)    :: t      !! Current simulation time
-         real(DP),                      intent(in)    :: dt     !! Step size
+         class(swiftest_parameters),    intent(in)    :: param !! Current run configuration parameters 
       end subroutine io_write_frame_system
 
-      module subroutine io_write_hdr(iu, t, npl, ntp, out_form, out_type)
-         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)
-      end subroutine io_write_hdr
-
       module subroutine obl_acc_body(self, cb)
          implicit none
          class(swiftest_body),         intent(inout) :: self !! Swiftest generic body object
@@ -633,7 +579,7 @@ end subroutine setup_body
       module subroutine setup_construct_system(system, param)
          implicit none
          class(swiftest_nbody_system),  allocatable,  intent(inout) :: system     !! Swiftest system object
-         type(swiftest_parameters),                intent(in)    :: param     !! Swiftest parameters parameters
+         type(swiftest_parameters),                intent(in)    :: param     !! Swiftest parameters
       end subroutine setup_construct_system
 
       module subroutine setup_pl(self,n)
@@ -655,13 +601,13 @@ end subroutine setup_set_msys
       module subroutine setup_set_mu_pl(self, cb)
          implicit none
          class(swiftest_pl),           intent(inout) :: self !! Swiftest massive body object
-         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body objectt
+         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body object
       end subroutine setup_set_mu_pl
 
       module subroutine setup_set_mu_tp(self, cb)
          implicit none
          class(swiftest_tp),           intent(inout) :: self !! Swiftest test particle object
-         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body objectt
+         class(swiftest_cb),           intent(inout) :: cb   !! Swiftest central body object
       end subroutine setup_set_mu_tp
 
       module subroutine setup_set_rhill(self,cb)
@@ -676,12 +622,12 @@ module subroutine setup_tp(self, n)
          integer,                      intent(in)    :: n    !! Number of bodies to allocate space for
       end subroutine setup_tp
 
-      module subroutine user_getacch_body(self, cb, param, t)
+      module subroutine user_getacch_body(self, system, param, t)
          implicit none
-         class(swiftest_body),          intent(inout) :: self   !! Swiftest massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
+         class(swiftest_body),         intent(inout) :: self   !! Swiftest massive body particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nobody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: t      !! Current time
       end subroutine user_getacch_body
 
       module subroutine util_coord_b2h_pl(self, cb)
@@ -710,7 +656,7 @@ end subroutine util_coord_h2b_tp
 
       module subroutine util_copy_body(self, src, mask)
          implicit none
-         class(swiftest_body),         intent(inout) :: self
+         class(swiftest_body),       intent(inout) :: self
          class(swiftest_base),       intent(in)    :: src
          logical, dimension(:),      intent(in)    :: mask
       end subroutine util_copy_body
@@ -722,7 +668,6 @@ module subroutine util_copy_cb(self, src, mask)
          logical, dimension(:),      intent(in)    :: mask
       end subroutine util_copy_cb
 
-
       module subroutine util_copy_pl(self, src, mask)
          implicit none
          class(swiftest_pl),         intent(inout) :: self
@@ -746,8 +691,8 @@ end subroutine util_copy_system
 
       module subroutine util_fill_body(self, inserts, lfill_list)
          implicit none
-         class(swiftest_body), intent(inout) :: self       !! Swiftest generic body object
-         class(swiftest_body), intent(inout) :: inserts     !! Insertted object 
+         class(swiftest_body),  intent(inout) :: self       !! Swiftest generic body object
+         class(swiftest_body),  intent(inout) :: inserts     !! Insertted object 
          logical, dimension(:), intent(in)   :: lfill_list  !! Logical array of bodies to merge into the keeps
       end subroutine util_fill_body
 
diff --git a/src/modules/symba.f90 b/src/modules/symba.f90
index bb0361d5c..82ff837a1 100644
--- a/src/modules/symba.f90
+++ b/src/modules/symba.f90
@@ -457,7 +457,7 @@ module subroutine symba_set_initial_conditions(symba_plA, symba_tpA, param)
       implicit none
       type(symba_pl), intent(inout) :: symba_plA  !! SyMBA massive body structure
       type(symba_tp), intent(inout) :: symba_tpA  !! SyMBA test particle structure
-      type(swiftest_parameters)  :: param     !! Input collection of on parameters
+      type(swiftest_parameters)  :: param     !! Current run configuration parameters of on parameters
    end subroutine symba_set_initial_conditions
 
    !> Method to remove the inactive symba test particles and spill them to a discard object
@@ -745,7 +745,7 @@ subroutine symba_encounter_dummy_input(self,param)
       !! This method is needed in order to extend the abstract type swiftest_body. It does nothing
       implicit none
       class(symba_encounter), intent(inout)  :: self  !! SyMBA encounter data structure 
-      type(swiftest_parameters),intent(in) :: param !! Input collection of on parameters
+      type(swiftest_parameters),intent(in) :: param !! Current run configuration parameters of on parameters
       return
    end subroutine symba_encounter_dummy_input
 
diff --git a/src/modules/whm_classes.f90 b/src/modules/whm_classes.f90
index 02e4c0806..031318161 100644
--- a/src/modules/whm_classes.f90
+++ b/src/modules/whm_classes.f90
@@ -9,19 +9,6 @@ module whm_classes
    implicit none
    public
 
-   !********************************************************************************************************************************
-   !  whm_nbody_system class definitions and method interfaces
-   !********************************************************************************************************************************
-   !> An abstract class for the WHM integrator nbody system 
-   type, public, extends(swiftest_nbody_system) :: whm_nbody_system
-      !> In the WHM integrator, only test particles are discarded
-      class(swiftest_tp), allocatable :: tp_discards
-   contains
-      private
-      !> Replace the abstract procedures with concrete ones
-      procedure, public :: initialize    => whm_setup_system  !! Performs WHM-specific initilization steps, like calculating the Jacobi masses
-      procedure, public :: step          => whm_step_system
-   end type whm_nbody_system
 
    !********************************************************************************************************************************
    ! whm_cb class definitions and method interfaces
@@ -71,8 +58,6 @@ module whm_classes
    type, public, extends(swiftest_tp) :: whm_tp
       !! Note to developers: If you add componenets to this class, be sure to update methods and subroutines that traverse the
       !!    component list, such as whm_setup_tp and whm_spill_tp
-      real(DP), dimension(:,:), allocatable :: xbeg, xend
-      logical                               :: beg
       logical                               :: lfirst = .true.
    contains
       private
@@ -82,200 +67,213 @@ module whm_classes
       procedure, public :: gr_p4        => whm_gr_p4_tp        !! Position kick due to p**4 term in the post-Newtonian correction
       procedure, public :: gr_vh2pv     => whm_gr_vh2pv_tp     !! Converts from heliocentric velocity to psudeovelocity for GR calculations
       procedure, public :: gr_pv2vh     => whm_gr_pv2vh_tp     !! Converts from psudeovelocity to heliocentric velocity for GR calculations
-      procedure, public :: set_beg_end  => whm_setup_set_beg_end     !! Sets the beginning and ending positions of planets.
       procedure, public :: setup        => whm_setup_tp        !! Allocates new components of the whm class and recursively calls parent allocations
       procedure, public :: step         => whm_step_tp         !! Steps the particle forward one stepsize
    end type whm_tp
 
-   interface
-      !> WHM massive body constructor method
-      module subroutine whm_setup_pl(self,n)
-         implicit none
-         class(whm_pl), intent(inout)    :: self !! Swiftest test particle object
-         integer(I4B),  intent(in)       :: n    !! Number of test particles to allocate
-      end subroutine whm_setup_pl
+   !********************************************************************************************************************************
+   !  whm_nbody_system class definitions and method interfaces
+   !********************************************************************************************************************************
+   !> An abstract class for the WHM integrator nbody system 
+   type, public, extends(swiftest_nbody_system) :: whm_nbody_system
+      !> In the WHM integrator, only test particles are discarded
+      class(whm_tp),            allocatable :: tp_discards   !! WHM test particle object that 
+      real(DP), dimension(:,:), allocatable :: xbeg, xend    !! Positions of massive bodies at beginning and end of a step. Required in order to separate the test particle step from the massive body step
+   contains
+      private
+      !> Replace the abstract procedures with concrete ones
+      procedure, public :: initialize   => whm_setup_system  !! Performs WHM-specific initilization steps, like calculating the Jacobi masses
+      procedure, public :: step         => whm_step_system
+      procedure, public :: set_beg_end  => whm_setup_set_beg_end     !! Sets the beginning and ending positions of planets.
+   end type whm_nbody_system
 
-      module subroutine whm_setup_set_mu_eta_pl(self, cb)
+   interface
+      module subroutine whm_coord_h2j_pl(self, cb)
          use swiftest_classes, only : swiftest_cb
          implicit none
-         class(whm_pl),                intent(inout) :: self    !! WHM massive body object
-         class(swiftest_cb),           intent(inout) :: cb     !! Swiftest central body object
-      end subroutine whm_setup_set_mu_eta_pl
-
-      module subroutine whm_setup_set_ir3j(self)
-         implicit none
-         class(whm_pl),                intent(inout) :: self    !! WHM massive body object
-      end subroutine whm_setup_set_ir3j
+         class(whm_pl),      intent(inout) :: self   !! WHM massive body particle data structure
+         class(swiftest_cb), intent(inout) :: cb     !! Swiftest central body particle data structuree
+      end subroutine whm_coord_h2j_pl
 
-      module subroutine whm_step_pl(self, cb, param, t, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine whm_coord_j2h_pl(self, cb)
+         use swiftest_classes, only : swiftest_cb
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! WHM massive body object
-         class(swiftest_cb),             intent(inout) :: cb     !! Swiftest central body particle data structure
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
-      end subroutine whm_step_pl
+         class(whm_pl),      intent(inout) :: self   !! WHM massive body particle data structure
+         class(swiftest_cb), intent(inout) :: cb     !! Swiftest central body particle data structuree
+      end subroutine whm_coord_j2h_pl
 
-      !> Get heliocentric accelration of massive bodies
-      module subroutine whm_getacch_pl(self, cb, param, t)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine whm_coord_vh2vj_pl(self, cb)
+         use swiftest_classes, only : swiftest_cb
          implicit none
-         class(whm_pl),                 intent(inout) :: self     !! WHM massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb       !! Swiftest central body particle data structure
-         class(swiftest_parameters), intent(in)    :: param   !! Input collection of 
-         real(DP),                      intent(in)    :: t        !! Current time
-      end subroutine whm_getacch_pl
+         class(whm_pl),      intent(inout) :: self   !! WHM massive body particle data structure
+         class(swiftest_cb), intent(inout) :: cb     !! Swiftest central body particle data structuree
+      end subroutine whm_coord_vh2vj_pl
 
-      module subroutine whm_drift_pl(self, cb, param, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine whm_drift_pl(self, system, param, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structur
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: dt     !! Stepsize
+         class(whm_pl),                intent(inout) :: self   !! WHM massive body particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: dt     !! Stepsize
       end subroutine whm_drift_pl
 
-      module subroutine whm_getacch_int_pl(self, cb)
-         use swiftest_classes, only : swiftest_cb
+      module subroutine whm_drift_tp(self, system, param, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),       intent(inout) :: cb     !! Swiftest central body particle data structure
-      end subroutine whm_getacch_int_pl
+         class(whm_tp),                intent(inout) :: self  !! WHM test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: dt    !! Stepsize
+      end subroutine whm_drift_tp
 
-      module subroutine whm_coord_h2j_pl(self, cb)
-         use swiftest_classes, only : swiftest_cb
+      module subroutine whm_fill_pl(self, inserts, lfill_list)
+         use swiftest_classes, only : swiftest_body
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),                 intent(inout) :: cb     !! Swiftest central body particle data structuree
-      end subroutine whm_coord_h2j_pl
+         class(whm_pl),         intent(inout) :: self       !! WHM massive body object
+         class(swiftest_body),  intent(inout) :: inserts    !! inserted object 
+         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
+      end subroutine whm_fill_pl
 
-      module subroutine whm_coord_j2h_pl(self, cb)
-         use swiftest_classes, only : swiftest_cb
+      !> Get heliocentric accelration of massive bodies
+      module subroutine whm_getacch_pl(self, system, param, t)
+         use swiftest_classes, only : swiftest_cb, swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),                 intent(inout) :: cb     !! Swiftest central body particle data structuree
-      end subroutine whm_coord_j2h_pl
+         class(whm_pl),                intent(inout) :: self   !! WHM massive body particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: t      !! Current simulation time
+      end subroutine whm_getacch_pl
 
-      module subroutine whm_coord_vh2vj_pl(self, cb)
-         use swiftest_classes, only : swiftest_cb
+      !> Get heliocentric accelration of the test particle
+      module subroutine whm_getacch_tp(self, system, param, t, xhp)
+         use swiftest_classes, only : swiftest_cb, swiftest_parameters
          implicit none
-         class(whm_pl),       intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),       intent(inout) :: cb     !! Swiftest central body particle data structuree
-      end subroutine whm_coord_vh2vj_pl
+         class(whm_tp),                intent(inout) :: self   !! WHM test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+         class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+         real(DP),                     intent(in)    :: t      !! Current time
+         real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets at the current substep
+      end subroutine whm_getacch_tp
 
-      module subroutine whm_gr_getacch_pl(self, cb, param)
+      module subroutine whm_gr_getacch_pl(self, param)
          use swiftest_classes, only : swiftest_cb, swiftest_parameters
          implicit none
-         class(whm_pl),       intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),  intent(inout) :: cb     !! Swiftest central body particle data structuree
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
+         class(whm_pl),              intent(inout) :: self  !! WHM massive body particle data structure
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of 
       end subroutine whm_gr_getacch_pl
 
+      module subroutine whm_gr_getacch_tp(self, param)
+         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+         implicit none
+         class(whm_tp),              intent(inout) :: self  !! WHM test particle data structure
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters
+      end subroutine whm_gr_getacch_tp
+
       module pure subroutine whm_gr_p4_pl(self, param, dt)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-         real(DP),                      intent(in)    :: dt     !! Step size
+         class(whm_pl),              intent(inout) :: self  !! Swiftest particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+         real(DP),                   intent(in)    :: dt    !! Step size
       end subroutine whm_gr_p4_pl
 
-      module pure subroutine whm_gr_vh2pv_pl(self, param)
+      module pure subroutine whm_gr_p4_tp(self, param, dt)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-      end subroutine whm_gr_vh2pv_pl
+         class(whm_tp),              intent(inout) :: self  !! WHM test particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+         real(DP),                    intent(in)   :: dt    !! Step size
+      end subroutine whm_gr_p4_tp
 
       module pure subroutine whm_gr_pv2vh_pl(self, param)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+         class(whm_pl),              intent(inout) :: self   !! Swiftest particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       end subroutine whm_gr_pv2vh_pl
 
-      !> WHM test particle constructor 
-      module subroutine whm_setup_tp(self,n)
+      module pure subroutine whm_gr_pv2vh_tp(self, param)
+         use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-         integer,                       intent(in)    :: n      !! Number of test particles to allocate
-      end subroutine whm_setup_tp
+         class(whm_tp),              intent(inout) :: self  !! WHM test particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+      end subroutine whm_gr_pv2vh_tp
 
-      module subroutine whm_drift_tp(self, cb, param, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module pure subroutine whm_gr_vh2pv_pl(self, param)
+         use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: dt     !! Stepsize
-      end subroutine whm_drift_tp
+         class(whm_pl),              intent(inout) :: self   !! Swiftest particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+      end subroutine whm_gr_vh2pv_pl
 
-      !> Get heliocentric accelration of the test particle
-      module subroutine whm_getacch_tp(self, cb, pl, param, t, xh)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module pure subroutine whm_gr_vh2pv_tp(self, param)
+         use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Generic Swiftest central body particle data structuree 
-         class(whm_pl),                 intent(inout) :: pl     !! WHM massive body particle data structure. 
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
-      end subroutine whm_getacch_tp
+         class(whm_tp),              intent(inout) :: self  !! WHM test particle object
+         class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+      end subroutine whm_gr_vh2pv_tp
 
-      module subroutine whm_step_tp(self, cb, pl, param, t, dt)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+
+      !> Reads WHM massive body object in from file
+      module subroutine whm_setup_pl(self,n)
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-         class(whm_pl),                 intent(inout) :: pl     !! WHM massive body data structure
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-         real(DP),                      intent(in)    :: t      !! Current time
-         real(DP),                      intent(in)    :: dt     !! Stepsize
-      end subroutine whm_step_tp
+         class(whm_pl), intent(inout)    :: self !! Swiftest test particle object
+         integer(I4B),  intent(in)       :: n    !! Number of test particles to allocate
+      end subroutine whm_setup_pl
 
       module subroutine whm_setup_set_beg_end(self, xbeg, xend, vbeg)
          implicit none
-         class(whm_tp),            intent(inout)          :: self !! Swiftest test particle object
+         class(whm_nbody_system),  intent(inout)          :: self !! WHM nbody system object
          real(DP), dimension(:,:), intent(in),   optional :: xbeg, xend
          real(DP), dimension(:,:), intent(in),   optional :: vbeg ! vbeg is an unused variable to keep this method forward compatible with RMVS
       end subroutine whm_setup_set_beg_end
 
-      module subroutine whm_gr_getacch_tp(self, cb, param)
-         use swiftest_classes, only : swiftest_cb, swiftest_parameters
+      module subroutine whm_setup_set_ir3j(self)
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! WHM massive body particle data structure
-         class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      end subroutine whm_gr_getacch_tp
+         class(whm_pl),                intent(inout) :: self    !! WHM massive body object
+      end subroutine whm_setup_set_ir3j
 
-      module pure subroutine whm_gr_p4_tp(self, param, dt)
-         use swiftest_classes, only : swiftest_parameters
+      module subroutine whm_setup_set_mu_eta_pl(self, cb)
+         use swiftest_classes, only : swiftest_cb
          implicit none
-         class(whm_tp),                 intent(inout) :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-         real(DP),                      intent(in)    :: dt     !! Step size
-      end subroutine whm_gr_p4_tp
+         class(whm_pl),                intent(inout) :: self    !! WHM massive body object
+         class(swiftest_cb),           intent(inout) :: cb     !! Swiftest central body object
+      end subroutine whm_setup_set_mu_eta_pl
 
-      module pure subroutine whm_gr_vh2pv_tp(self, param)
+      module subroutine whm_setup_system(self, param)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_tp),                 intent(inout)    :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-      end subroutine whm_gr_vh2pv_tp
+         class(whm_nbody_system),    intent(inout) :: self   !! WHM nbody system object
+         class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters of on parameters 
+      end subroutine whm_setup_system
 
-      module pure subroutine whm_gr_pv2vh_tp(self, param)
-         use swiftest_classes, only : swiftest_parameters
+      !> Reads WHM test particle object in from file
+      module subroutine whm_setup_tp(self,n)
          implicit none
-         class(whm_tp),                 intent(inout)    :: self   !! Swiftest particle object
-         class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-      end subroutine whm_gr_pv2vh_tp
+         class(whm_tp), intent(inout) :: self   !! WHM test particle data structure
+         integer,       intent(in)    :: n      !! Number of test particles to allocate
+      end subroutine whm_setup_tp
 
-      module subroutine whm_setup_system(self, param)
-         use swiftest_classes, only : swiftest_parameters
+      module subroutine whm_step_pl(self, system, param, t, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
          implicit none
-         class(whm_nbody_system),       intent(inout) :: self    !! Swiftest system object
-         class(swiftest_parameters), intent(inout) :: param  !! Input collection of on parameters 
-      end subroutine whm_setup_system
+         class(whm_pl),                intent(inout) :: self   !! WHM massive 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
+      end subroutine whm_step_pl
+
+      module subroutine whm_step_tp(self, system, param, t, dt)
+         use swiftest_classes, only : swiftest_nbody_system, swiftest_parameters
+         implicit none
+         class(whm_tp),                intent(inout) :: self   !! WHM test particle data structure
+         class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody system object
+         class(swiftest_parameters),   intent(inout) :: param  !! Current run configuration parameters
+         real(DP),                     intent(in)    :: t      !! Current simulation time
+         real(DP),                     intent(in)    :: dt     !! Stepsize
+      end subroutine whm_step_tp
 
       module subroutine whm_spill_pl(self, discards, lspill_list)
          use swiftest_classes, only : swiftest_body
@@ -285,20 +283,14 @@ module subroutine whm_spill_pl(self, discards, lspill_list)
          logical, dimension(:), intent(in)    :: lspill_list !! Logical array of bodies to spill into the discards
       end subroutine whm_spill_pl
 
-      module subroutine whm_fill_pl(self, inserts, lfill_list)
-         use swiftest_classes, only : swiftest_body
-         implicit none
-         class(whm_pl),         intent(inout) :: self       !! WHM massive body object
-         class(swiftest_body),  intent(inout) :: inserts    !! inserted object 
-         logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
-      end subroutine whm_fill_pl
-
       !> Steps the Swiftest nbody system forward in time one stepsize
-      module subroutine whm_step_system(self, param)
+      module subroutine whm_step_system(self, param, t, dt)
          use swiftest_classes, only : swiftest_parameters
          implicit none
-         class(whm_nbody_system),       intent(inout) :: self    !! WHM system object
-         class(swiftest_parameters), intent(in)    :: param  !! Input collection of on parameters 
+         class(whm_nbody_system),    intent(inout) :: self    !! WHM 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
       end subroutine whm_step_system
    end interface
 
diff --git a/src/obl/obl.f90 b/src/obl/obl.f90
index 1a6b77d09..1192189df 100644
--- a/src/obl/obl.f90
+++ b/src/obl/obl.f90
@@ -1,7 +1,7 @@
 submodule (swiftest_classes) s_obl
    use swiftest
 contains
-   module procedure obl_acc_body 
+   module subroutine obl_acc_body(self, cb)
       !! author: David A. Minton
       !!
       !! Compute the barycentric accelerations of bodies due to the oblateness of the central body
@@ -10,39 +10,40 @@
       !! Adapted from David E. Kaufmann's Swifter routine: obl_acc.f90 and obl_acc_tp.f90
       !! Adapted from Hal Levison's Swift routine obl_acc.f and obl_acc_tp.f
       implicit none
+      ! Arguments
+      class(swiftest_body), intent(inout) :: self !! Swiftest generic body object
+      class(swiftest_cb),   intent(inout) :: cb   !! Swiftest central body object
+      ! Internals
       integer(I4B) :: i
       real(DP)     :: r2, irh, rinv2, t0, t1, t2, t3, fac1, fac2
 
-      associate(n => self%nbody, aobl => self%aobl, xh => self%xh, j2rp2 => cb%j2rp2, j4rp4 => cb%j4rp4, &
-                msun => cb%Gmass, aoblcb => cb%aobl, ah => self%ah)
+      associate(n => self%nbody, xh => self%xh, vh => self%vh, ah => self%ah)
          do i = 1, n 
-            r2 = dot_product(xh(:, i), xh(:, i))
+            r2 = dot_product(self%xh(:, i), self%xh(:, i))
             irh = 1.0_DP / sqrt(r2)
             rinv2 = irh**2
-            t0 = -msun * rinv2*rinv2*irh
-            t1 = 1.5_DP * j2rp2
-            t2 = xh(3, i) * xh(3, i) * rinv2
-            t3 = 1.875_DP * j4rp4 * rinv2
-            fac1 = t0 * (t1 - t3 - (5.0_DP * t1 - (14.0_DP - 21.0_DP * t2) * t3) * t2)
-            fac2 = 2.0_DP * t0 * (t1 - (2.0_DP - (14.0_DP * t2 / 3.0_DP)) * t3)
-            aobl(:, i) = fac1 * xh(:, i)
-            aobl(3, i) = fac2 * xh(3, i) + aobl(3, i)
+            t0 = -cb%Gmass * rinv2 * rinv2 * irh
+            t1 = 1.5_DP * cb%j2rp2
+            t2 = self%xh(3, i) * self%xh(3, i) * rinv2
+            t3 = 1.875_DP * cb%j4rp4 * rinv2
+            fac1 = t0 * (t1 - t3 - (5 * t1 - (14.0_DP - 21.0_DP * t2) * t3) * t2)
+            fac2 = 2 * t0 * (t1 - (2.0_DP - (14.0_DP * t2 / 3.0_DP)) * t3)
+            self%aobl(:, i) = fac1 * self%xh(:, i)
+            self%aobl(3, i) = fac2 * self%xh(3, i) + self%aobl(3, i)
          end do
          select type(self)
          class is (swiftest_pl)
-            associate(Mpl => self%Gmass)
-               do i = 1, NDIM
-                  aoblcb(i) = -sum(Mpl(1:n) * aobl(i, 1:n)) / msun
-               end do
-            end associate
+            do i = 1, NDIM
+               cb%aobl(i) = -sum(self%Gmass(1:n) * self%aobl(i, 1:n)) / cb%Gmass
+            end do
          end select
 
          do i = 1, NDIM
-            ah(i, 1:n) = ah(i, 1:n) + aobl(i, 1:n) - aoblcb(i)
+            self%ah(i, 1:n) = self%ah(i, 1:n) + self%aobl(i, 1:n) - cb%aobl(i)
          end do
       end associate
       return
 
-   end procedure obl_acc_body
+   end subroutine obl_acc_body
 
 end submodule s_obl
diff --git a/src/rmvs/rmvs_discard.f90 b/src/rmvs/rmvs_discard.f90
index 4f75cd645..dc8b4b9bb 100644
--- a/src/rmvs/rmvs_discard.f90
+++ b/src/rmvs/rmvs_discard.f90
@@ -1,7 +1,7 @@
 submodule(rmvs_classes) s_rmvs_discard
    use swiftest
 contains  
-   module subroutine rmvs_discard_pl_tp(self, pl, t, dt)
+   module subroutine rmvs_discard_pl_tp(self, system, param)
       !! author: David A. Minton
       !!
       !! Check to see if test particles should be discarded based on pericenter passage distances with respect to
@@ -11,14 +11,13 @@ module subroutine rmvs_discard_pl_tp(self, pl, t, dt)
       !! Adapted from Hal Levison's Swift routine rmvs_discard_pl.f90
       implicit none
       ! Arguments
-      class(rmvs_tp),                intent(inout) :: self
-      class(swiftest_pl),            intent(inout) :: pl     !! WHM massive body particle data structure. 
-      real(DP),                      intent(in)    :: t      !! Current simulation time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(rmvs_tp),               intent(inout) :: self   !! RMVS 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
       integer(I4B)                                 :: i
 
-      associate(tp => self, ntp => self%nbody)
+      associate(tp => self, ntp => self%nbody, pl => system%pl, t => param%t)
          do i = 1, ntp
             associate(iplperP => tp%plperP(i))
                if ((tp%status(i) == ACTIVE) .and. (tp%lperi(i))) then 
@@ -30,7 +29,7 @@ module subroutine rmvs_discard_pl_tp(self, pl, t, dt)
                end if
             end associate
          end do
-         call discard_pl_tp(tp, pl, t, dt)
+         call discard_pl_tp(tp, system, param)
       end associate
 
    end subroutine rmvs_discard_pl_tp
diff --git a/src/rmvs/rmvs_encounter_check.f90 b/src/rmvs/rmvs_encounter_check.f90
index 3d5543166..9719567a9 100644
--- a/src/rmvs/rmvs_encounter_check.f90
+++ b/src/rmvs/rmvs_encounter_check.f90
@@ -1,7 +1,7 @@
 submodule (rmvs_classes) s_rmvs_chk
    use swiftest
 contains
-   module function rmvs_encounter_check_tp(self, cb, pl, dt, rts) result(lencounter)
+   module function rmvs_encounter_check_tp(self, system, dt) result(lencounter)
       !! author: David A. Minton
       !!
       !! Determine whether a test particle and planet are having or will have an encounter within the next time step
@@ -10,38 +10,39 @@ module function rmvs_encounter_check_tp(self, cb, pl, dt, rts) result(lencounter
       !! Adapted from Hal Levison's Swift routine rmvs3_chk.f
       implicit none
       ! Arguments
-      class(rmvs_tp),            intent(inout) :: self        !! RMVS test particle object  
-      class(rmvs_cb),            intent(inout) :: cb          !! RMVS central body object  
-      class(rmvs_pl),       intent(inout) :: pl          !! RMVS massive body object  
-      real(DP),                  intent(in)    :: dt          !! step size
-      real(DP),                  intent(in)    :: rts         !! fraction of Hill's sphere radius to use as radius of encounter regio
-      logical                                  :: lencounter  !! Returns true if there is at least one close encounter
+      class(rmvs_tp),           intent(inout) :: self   !! RMVS test particle object  
+      class(rmvs_nbody_system), intent(inout) :: system !! RMVS nbody system object
+      real(DP),                 intent(in)    :: dt     !! step size
+      ! Result
+      logical                                 :: lencounter  !! Returns true if there is at least one close encounter
       ! Internals
-      integer(I4B)                             :: i, j
-      real(DP)                                 :: r2, v2, vdotr
-      real(DP), dimension(NDIM)                :: xr, vr
-      real(DP), dimension(pl%nbody)            :: r2crit
-      logical                                  :: lflag
+      integer(I4B)                            :: i, j
+      real(DP)                                :: r2, v2, vdotr
+      real(DP), dimension(NDIM)               :: xr, vr
+      real(DP), dimension(system%pl%nbody)    :: r2crit
+      logical                                 :: lflag
 
-      associate(tp => self, ntp => self%nbody, npl => pl%nbody, rhill => pl%rhill, xht => self%xh, vht => self%vh, &
-                 xbeg => self%xbeg, vbeg => self%vbeg, status => self%status, plencP => self%plencP, nenc => pl%nenc)
-         r2crit(:) = (rts * rhill(:))**2
-         plencP(:) = 0
-         do j = 1, npl
-            do i = 1, ntp
-               if ((status(i) /= ACTIVE).or.(plencP(i) /= 0)) cycle
-               xr(:) = xht(:, i) - xbeg(:, j)
-               vr(:) = vht(:, i) - vbeg(:, j)
-               r2 = dot_product(xr(:), xr(:))
-               v2 = dot_product(vr(:), vr(:))
-               vdotr = dot_product(vr(:), xr(:))
-               lflag = rmvs_chk_ind(r2, v2, vdotr, dt, r2crit(j))
-               if (lflag) plencP(i) = j
+      select type(pl => system%pl)
+      class is (rmvs_pl)
+         associate(tp => self, ntp => self%nbody, npl => pl%nbody, xbeg => system%xbeg, vbeg => system%vbeg, rts => system%rts)
+            r2crit(:) = (rts * pl%rhill(:))**2
+            tp%plencP(:) = 0
+            do j = 1, npl
+               do i = 1, ntp
+                  if ((tp%status(i) /= ACTIVE).or.(tp%plencP(i) /= 0)) cycle
+                  xr(:) = tp%xh(:, i) - xbeg(:, j)
+                  vr(:) = tp%vh(:, i) - vbeg(:, j)
+                  r2 = dot_product(xr(:), xr(:))
+                  v2 = dot_product(vr(:), vr(:))
+                  vdotr = dot_product(vr(:), xr(:))
+                  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)
             end do
-            nenc(j) = count(plencP(:) == j)
-         end do
-         lencounter = any(nenc(:) > 0)
-      end associate
+            lencounter = any(pl%nenc(:) > 0)
+         end associate
+      end select
       return
    end function rmvs_encounter_check_tp
 
diff --git a/src/rmvs/rmvs_getacch.f90 b/src/rmvs/rmvs_getacch.f90
index 6201c42da..dcbf5aff9 100644
--- a/src/rmvs/rmvs_getacch.f90
+++ b/src/rmvs/rmvs_getacch.f90
@@ -1,7 +1,8 @@
 submodule(rmvs_classes) s_rmvs_getacch
    use swiftest
 contains  
-   module subroutine rmvs_getacch_tp(self, cb, pl, param, t, xh)
+   module subroutine rmvs_getacch_tp(self, system, param, t, xhp)
+
       !! author: David A. Minton
       !!
       !! Compute the oblateness acceleration in the inner encounter region with planets 
@@ -10,69 +11,69 @@ module subroutine rmvs_getacch_tp(self, cb, pl, param, t, xh)
       !! uses object polymorphism, and so is not directly adapted.
       implicit none
       ! Arguments
-      class(rmvs_tp),                intent(inout) :: self   !! RMVS test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree 
-      class(whm_pl),                 intent(inout) :: pl     !! WHM massive body particle data structure. 
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of  parameter
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
+      class(rmvs_tp),               intent(inout) :: self   !! RMVS test particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! Swiftest central body particle data structuree 
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters
+      real(DP),                     intent(in)    :: t      !! Current time
+      real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets at current substep
       ! Internals
       type(swiftest_parameters)                 :: param_planetocen
       real(DP), dimension(:, :), allocatable       :: xh_original
       integer(I4B)                                 :: i
 
 
-      associate(tp => self, ntp => self%nbody, ipleP => self%ipleP, &
-                inner_index => self%index, cb_heliocentric => self%cb_heliocentric)
-         
-         if (tp%lplanetocentric) then  ! This is a close encounter step, so any accelerations requiring heliocentric position values
-                                       ! must be handeled outside the normal WHM method call
-            select type(pl)
-            class is (rmvs_pl)
-            select type (cb)
-            class is (rmvs_cb)
-               associate(xpc => pl%xh, xpct => self%xh)
-                  allocate(xh_original, source=tp%xh)
-                  param_planetocen = param
-                  ! Temporarily turn off the heliocentric-dependent acceleration terms during an inner encounter
-                  param_planetocen%loblatecb = .false.
-                  param_planetocen%lextra_force = .false.
-                  param_planetocen%lgr = .false.
-                  ! Now compute the planetocentric values of acceleration
-                  call whm_getacch_tp(tp, cb, pl, param_planetocen, t, xh)
+      associate(tp => self, ntp => self%nbody, ipleP => self%ipleP, inner_index => self%index, cb_heliocentric => self%cb_heliocentric)
+         select type(system)
+         class is (rmvs_nbody_system)
+            if (system%lplanetocentric) then  ! This is a close encounter step, so any accelerations requiring heliocentric position values
+                                          ! must be handeled outside the normal WHM method call
+               select type(pl => system%pl)
+               class is (rmvs_pl)
+               select type (cb => system%cb)
+               class is (rmvs_cb)
+                  associate(xpc => pl%xh, xpct => self%xh, apct => self%ah)
+                     allocate(xh_original, source=tp%xh)
+                     param_planetocen = param
+                     ! Temporarily turn off the heliocentric-dependent acceleration terms during an inner encounter
+                     param_planetocen%loblatecb = .false.
+                     param_planetocen%lextra_force = .false.
+                     param_planetocen%lgr = .false.
+                     ! Now compute the planetocentric values of acceleration
+                     call whm_getacch_tp(tp, system, param_planetocen, t, xhp)
 
-                  ! Now compute any heliocentric values of acceleration 
-                  if (tp%lfirst) then
-                     do i = 1, ntp
-                        tp%xheliocentric(:,i) = tp%xh(:,i) + cb%inner(inner_index - 1)%x(:,1)
-                     end do
-                  else
-                     do i = 1, ntp
-                        tp%xheliocentric(:,i) = tp%xh(:,i) + cb%inner(inner_index    )%x(:,1)
-                     end do
-                  end if
-                  ! Swap the planetocentric and heliocentric position vectors
-                  tp%xh(:,:) = tp%xheliocentric(:,:)
-                  if (param%loblatecb) then
-                     ! Put in the current encountering planet's oblateness acceleration as the central body's
+                     ! Now compute any heliocentric values of acceleration 
                      if (tp%lfirst) then
-                        cb_heliocentric%aobl(:) = cb%inner(inner_index - 1)%aobl(:,1)
+                        do i = 1, ntp
+                           tp%xheliocentric(:,i) = tp%xh(:,i) + cb%inner(inner_index - 1)%x(:,1)
+                        end do
                      else
-                        cb_heliocentric%aobl(:) = cb%inner(inner_index    )%aobl(:,1)
+                        do i = 1, ntp
+                           tp%xheliocentric(:,i) = tp%xh(:,i) + cb%inner(inner_index    )%x(:,1)
+                        end do
+                     end if
+                     ! Swap the planetocentric and heliocentric position vectors
+                     tp%xh(:,:) = tp%xheliocentric(:,:)
+                     if (param%loblatecb) then
+                        ! Put in the current encountering planet's oblateness acceleration as the central body's
+                        if (tp%lfirst) then
+                           cb_heliocentric%aobl(:) = cb%inner(inner_index - 1)%aobl(:,1)
+                        else
+                           cb_heliocentric%aobl(:) = cb%inner(inner_index    )%aobl(:,1)
+                        end if
+                        call tp%obl_acc(cb_heliocentric)
                      end if
-                     call tp%obl_acc(cb_heliocentric)
-                  end if
 
-                  if (param%lextra_force) call tp%user_getacch(cb_heliocentric, param, t)
-                  if (param%lgr) call tp%gr_getacch(cb_heliocentric, param)
-                  
-                  tp%xh(:,:) = xh_original(:,:)
-               end associate
-            end select
-            end select
-         else ! Not a close encounter, so just proceded with the standard WHM method
-            call whm_getacch_tp(tp, cb, pl, param, t, xh)
-         end if
+                     if (param%lextra_force) call tp%user_getacch(system, param, t)
+                     if (param%lgr) call tp%gr_getacch(param)
+                     
+                     tp%xh(:,:) = xh_original(:,:)
+                  end associate
+               end select
+               end select
+            else ! Not a close encounter, so just proceded with the standard WHM method
+               call whm_getacch_tp(tp, system, param, t, xhp)
+            end if
+         end select
 
       end associate
 
diff --git a/src/rmvs/rmvs_setup.f90 b/src/rmvs/rmvs_setup.f90
index 95634e0a1..9d5916f56 100644
--- a/src/rmvs/rmvs_setup.f90
+++ b/src/rmvs/rmvs_setup.f90
@@ -9,7 +9,7 @@ module subroutine rmvs_setup_pl(self,n)
       !! Equivalent in functionality to David E. Kaufmann's Swifter routine rmvs_setup.f90
       implicit none
       ! Arguments
-      class(rmvs_base_pl),           intent(inout) :: self !! RMVS test particle object
+      class(rmvs_pl),           intent(inout) :: self !! RMVS test particle object
       integer(I4B),                  intent(in)    :: n    !! Number of test particles to allocate
       ! Internals
       integer(I4B)                                 :: i,j
@@ -24,7 +24,7 @@ module subroutine rmvs_setup_pl(self,n)
          allocate(pl%inner(0:NTPHENC))
          if (.not.pl%lplanetocentric) then
             allocate(pl%nenc(n))
-            pl%nenc(:)         = 0
+            pl%nenc(:) = 0
 
             ! Set up inner and outer planet interpolation vector storage containers
             do i = 0, NTENC
@@ -86,7 +86,7 @@ module subroutine rmvs_setup_system(self, param)
       implicit none
       ! Arguments
       class(rmvs_nbody_system),      intent(inout) :: self    !! RMVS system object
-      class(swiftest_parameters), intent(inout) :: param  !! Input collection of  parameters parameters 
+      class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters 
       ! Internals
       integer(I4B) :: i, j
 
@@ -97,46 +97,50 @@ module subroutine rmvs_setup_system(self, param)
       ! generated as necessary during close encounter steps.
       select type(pl => self%pl)
       class is(rmvs_pl)
-      select type(cb => self%cb)
-      class is (rmvs_cb)
-      select type (tp => self%tp)
-      class is (rmvs_tp)
-         tp%cb_heliocentric = cb
-         pl%lplanetocentric = .false.
-         tp%lplanetocentric = .false.
-         cb%lplanetocentric = .false.
-         associate(npl => pl%nbody)
-            allocate(pl%planetocentric(npl))
-            do i = 1, npl
-               allocate(pl%planetocentric(i)%cb, source=cb)
-               allocate(rmvs_pl :: pl%planetocentric(i)%pl)
-               associate(plenci => pl%planetocentric(i)%pl, cbenci => pl%planetocentric(i)%cb)
-                  cbenci%lplanetocentric = .true.
-                  plenci%lplanetocentric = .true.
-                  call plenci%setup(npl)
-                  plenci%status(:) = ACTIVE
-
-                  ! plind stores the heliocentric index value of a planetocentric planet
-                  ! e.g. Consider an encounter with planet 3.  
-                  ! Then the following will be the values of plind:
-                  ! pl%planetocentric(3)%pl%plind(1) = 0 (central body - never used)  
-                  ! pl%planetocentric(3)%pl%plind(2) = 1  
-                  ! pl%planetocentric(3)%pl%plind(3) = 2
-                  ! pl%planetocentric(3)%pl%plind(4) = 4
-                  ! pl%planetocentric(3)%pl%plind(5) = 5
-                  ! etc.  
-                  allocate(plenci%plind(npl))
-                  plenci%plind(1:npl) = [(j,j=1,npl)] 
-                  plenci%plind(2:npl) = pack(plenci%plind(1:npl), plenci%plind(1:npl) /= i)
-                  plenci%plind(1)     = 0
-                  plenci%Gmass(1)     = cb%Gmass
-                  plenci%Gmass(2:npl) = pl%Gmass(plenci%plind(2:npl))
-                  cbenci%Gmass        = pl%Gmass(i)
+         select type(cb => self%cb)
+         class is (rmvs_cb)
+            select type (tp => self%tp)
+            class is (rmvs_tp)
+               tp%cb_heliocentric = cb
+               pl%lplanetocentric = .false.
+               tp%lplanetocentric = .false.
+               cb%lplanetocentric = .false.
+               associate(npl => pl%nbody)
+                  allocate(pl%planetocentric(npl))
+                  pl%planetocentric(:)%lplanetocentric = .true.
+                  do i = 1, npl
+                     allocate(pl%planetocentric(i)%cb, source=cb)
+                     allocate(rmvs_pl :: pl%planetocentric(i)%pl)
+                     select type(cbenci => pl%planetocentric(i)%cb)
+                     class is (rmvs_cb)
+                        select type(plenci => pl%planetocentric(i)%pl)
+                        class is (rmvs_pl)
+                           cbenci%lplanetocentric = .true.
+                           plenci%lplanetocentric = .true.
+                           call plenci%setup(npl)
+                           plenci%status(:) = ACTIVE
+                           ! plind stores the heliocentric index value of a planetocentric planet
+                           ! e.g. Consider an encounter with planet 3.  
+                           ! Then the following will be the values of plind:
+                           ! pl%planetocentric(3)%pl%plind(1) = 0 (central body - never used)  
+                           ! pl%planetocentric(3)%pl%plind(2) = 1  
+                           ! pl%planetocentric(3)%pl%plind(3) = 2
+                           ! pl%planetocentric(3)%pl%plind(4) = 4
+                           ! pl%planetocentric(3)%pl%plind(5) = 5
+                           ! etc.  
+                           allocate(plenci%plind(npl))
+                           plenci%plind(1:npl) = [(j,j=1,npl)] 
+                           plenci%plind(2:npl) = pack(plenci%plind(1:npl), plenci%plind(1:npl) /= i)
+                           plenci%plind(1)     = 0
+                           plenci%Gmass(1)     = cb%Gmass
+                           plenci%Gmass(2:npl) = pl%Gmass(plenci%plind(2:npl))
+                           cbenci%Gmass        = pl%Gmass(i)
+                        end select
+                     end select
+                  end do
                end associate
-            end do
-         end associate
-      end select
-      end select
+            end select
+         end select
       end select
    
    end subroutine rmvs_setup_system
@@ -147,7 +151,7 @@ module subroutine rmvs_setup_set_beg_end(self, xbeg, xend, vbeg)
       !! Sets one or more of the values of xbeg, xend, and vbeg
       implicit none
       ! Arguments
-      class(rmvs_tp),           intent(inout)          :: self !! RMVS test particle object
+      class(rmvs_nbody_system), intent(inout)          :: self !! RMVS test particle object
       real(DP), dimension(:,:), intent(in),   optional :: xbeg, xend, vbeg
 
       if (present(xbeg)) then
diff --git a/src/rmvs/rmvs_spill_and_fill.f90 b/src/rmvs/rmvs_spill_and_fill.f90
index 4eb1e81dc..ae0ff563b 100644
--- a/src/rmvs/rmvs_spill_and_fill.f90
+++ b/src/rmvs/rmvs_spill_and_fill.f90
@@ -9,9 +9,9 @@ module subroutine rmvs_spill_pl(self, discards, lspill_list)
       !! Adapted from David E. Kaufmann's Swifter routine discard_discard_spill.f90
       implicit none
       ! Arguments
-      class(rmvs_base_pl),                   intent(inout) :: self      !! Swiftest massive body body object
-      class(swiftest_body),                  intent(inout) :: discards    !! Discarded object 
-      logical, dimension(:),                 intent(in)    :: lspill_list !! Logical array of bodies to spill into the discards
+      class(rmvs_pl),        intent(inout) :: self      !! Swiftest massive body body object
+      class(swiftest_body),  intent(inout) :: discards    !! Discarded object 
+      logical, dimension(:), intent(in)    :: lspill_list !! Logical array of bodies to spill into the discards
       ! Internals
       integer(I4B)                                         :: i
 
@@ -41,7 +41,7 @@ module subroutine rmvs_fill_pl(self, inserts, lfill_list)
          !! 
          implicit none
          ! Arguments
-         class(rmvs_base_pl),   intent(inout) :: self       !! RMVS massive body object
+         class(rmvs_pl),        intent(inout) :: self       !! RMVS massive body object
          class(swiftest_body),  intent(inout) :: inserts    !! Inserted object 
          logical, dimension(:), intent(in)    :: lfill_list !! Logical array of bodies to merge into the keeps
          ! Internals
diff --git a/src/rmvs/rmvs_step.f90 b/src/rmvs/rmvs_step.f90
index 4d864e807..3336d3e98 100644
--- a/src/rmvs/rmvs_step.f90
+++ b/src/rmvs/rmvs_step.f90
@@ -1,7 +1,7 @@
 submodule(rmvs_classes) s_rmvs_step
    use swiftest
 contains
-   module subroutine rmvs_step_system(self, param)
+   module subroutine rmvs_step_system(self, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step massive bodies and and active test particles ahead in heliocentric coordinates
@@ -10,60 +10,60 @@ module subroutine rmvs_step_system(self, param)
       !! Adapted from David E. Kaufmann's Swifter routine rmvs_step.f90
       implicit none
       ! Arguments
-      class(rmvs_nbody_system),          intent(inout)  :: self    !! RMVS nbody system object
-      class(swiftest_parameters),     intent(in)     :: param  !! Input collection of  parameters parameters 
+      class(rmvs_nbody_system),   intent(inout)  :: self   !! RMVS nbody system object
+      class(swiftest_parameters), intent(inout)  :: param  !! Current run configuration parameters 
+      real(DP),                   intent(in)    :: t     !! Current simulation time
+      real(DP),                   intent(in)    :: dt    !! Current stepsiz
       ! Internals
       logical :: lencounter, lfirstpl, lfirsttp 
       real(DP) :: rts
       real(DP), dimension(:,:), allocatable :: xbeg, xend, vbeg
       integer(I4B) :: i
- 
+
       select type(cb => self%cb)
       class is (rmvs_cb)
-      select type(pl => self%pl)
-      class is (rmvs_pl)
-      select type(tp => self%tp)
-      class is (rmvs_tp)
-      associate(ntp => tp%nbody, npl => pl%nbody, t => param%t, dt => param%dt, &
-         xhpl => pl%xh, vhpl => pl%vh, xjpl => pl%xj, vjpl => pl%vj, &
-         xhtp => tp%xh, vhtp => tp%vh)
-         allocate(xbeg, source=pl%xh)
-         allocate(vbeg, source=pl%vh)
-         call pl%set_rhill(cb)
-         call tp%set_beg_end(xbeg = xbeg, vbeg = vbeg)
-         ! ****** Check for close encounters ***** !
-         rts = RHSCALE
-         lencounter = tp%encounter_check(cb, pl, dt, rts)
-         if (lencounter) then
-            lfirstpl = pl%lfirst
-            lfirsttp = tp%lfirst
-            pl%outer(0)%x(:,:) = xbeg(:,:)
-            pl%outer(0)%v(:,:) = vbeg(:,:)
-            call pl%step(cb, param, t, dt) 
-            pl%outer(NTENC)%x(:,:) = pl%xh(:,:)
-            pl%outer(NTENC)%v(:,:) = pl%vh(:,:)
-            call tp%set_beg_end(xend = pl%xh)
-            call rmvs_interp_out(pl,cb, dt, param)
-            call rmvs_step_out(pl, cb, tp, dt, param)
-            call tp%reverse_status()
-            call tp%set_beg_end(xbeg = xbeg, xend = xend)
-            tp%lfirst = .true.
-            call tp%step(cb, pl, param, t, dt)
-            where (tp%status(:) == INACTIVE) tp%status(:) = ACTIVE
-            pl%lfirst = lfirstpl
-            tp%lfirst = lfirsttp
-         else
-            call whm_step_system(self, param)
-         end if
-      end associate
-      end select
-      end select
+         select type(pl => self%pl)
+         class is (rmvs_pl)
+            select type(tp => self%tp)
+            class is (rmvs_tp)
+               associate(system => self, ntp => tp%nbody, npl => pl%nbody)
+                  allocate(xbeg, source=pl%xh)
+                  allocate(vbeg, source=pl%vh)
+                  call pl%set_rhill(cb)
+                  call system%set_beg_end(xbeg = xbeg, vbeg = vbeg)
+                  ! ****** Check for close encounters ***** !
+                  system%rts = RHSCALE
+                  lencounter = tp%encounter_check(system, dt)
+                  if (lencounter) then
+                     lfirstpl = pl%lfirst
+                     lfirsttp = tp%lfirst
+                     pl%outer(0)%x(:,:) = xbeg(:,:)
+                     pl%outer(0)%v(:,:) = vbeg(:,:)
+                     call pl%step(system, param, t, dt) 
+                     pl%outer(NTENC)%x(:,:) = pl%xh(:,:)
+                     pl%outer(NTENC)%v(:,:) = pl%vh(:,:)
+                     call system%set_beg_end(xend = pl%xh)
+                     call rmvs_interp_out(system, param, dt)
+                     call rmvs_step_out(system, param, t, dt) 
+                     call tp%reverse_status()
+                     call system%set_beg_end(xbeg = xbeg, xend = xend)
+                     tp%lfirst = .true.
+                     call tp%step(system, param, t, dt)
+                     where (tp%status(:) == INACTIVE) tp%status(:) = ACTIVE
+                     pl%lfirst = lfirstpl
+                     tp%lfirst = lfirsttp
+                  else
+                     call whm_step_system(self, param, t, dt)
+                  end if
+               end associate
+            end select
+         end select
       end select
       return
 
    end subroutine rmvs_step_system 
 
-   subroutine rmvs_step_out(pl, cb, tp, dt, param)
+   subroutine rmvs_step_out(system, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step ACTIVE test particles ahead in the outer encounter region, setting up and calling the inner region
@@ -73,53 +73,58 @@ subroutine rmvs_step_out(pl, cb, tp, dt, param)
       !! Adapted from David E. Kaufmann's Swifter routines rmvs_step_out.f90 and rmvs_step_out2.f90
       implicit none
       ! Arguments
-      class(rmvs_pl),                    intent(inout)  :: pl !! RMVS massive body object
-      class(rmvs_cb),                    intent(inout)  :: cb   !! RMVS central body object
-      class(rmvs_tp),                    intent(inout)  :: tp   !! RMVS test particle object
-      real(DP),                          intent(in)     :: dt   !! Step size
-      class(swiftest_parameters),     intent(in)     :: param  !! Input collection of  parameters parameters
+      class(rmvs_nbody_system),   intent(inout) :: system !! Swiftest system object
+      class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters 
+      real(DP),                   intent(in)    :: t     !! Current simulation time
+      real(DP),                   intent(in)    :: dt    !! Current stepsiz
       ! Internals
-      integer(I4B)                                      :: outer_index, j, k
-      real(DP)                                          :: dto, outer_time, rts
-      logical                                           :: lencounter, lfirsttp
+      integer(I4B)                              :: outer_index, j, k
+      real(DP)                                  :: dto, outer_time, rts
+      logical                                   :: lencounter, lfirsttp
 
-      associate(npl => pl%nbody, ntp => tp%nbody, t => param%t)
-         dto = dt / NTENC
-         where(tp%plencP(:) == 0)
-            tp%status(:) = INACTIVE
-         elsewhere  
-            tp%lperi(:) = .false.
-         end where
-         do outer_index = 1, NTENC
-            outer_time = t + (outer_index - 1) * dto
-            call tp%set_beg_end(xbeg = pl%outer(outer_index - 1)%x(:, :), &
-                                vbeg = pl%outer(outer_index - 1)%v(:, :), &
-                                xend = pl%outer(outer_index    )%x(:, :))
-            rts = RHPSCALE
-            lencounter = tp%encounter_check(cb, pl, dt, rts) 
-            if (lencounter) then
-               ! Interpolate planets in inner encounter region
-               call rmvs_interp_in(pl, cb, dto, outer_index, param)
-               ! Step through the inner region
-               call rmvs_step_in(pl, cb, tp, param, outer_time, dto)
-               lfirsttp = tp%lfirst
-               tp%lfirst = .true.
-               call tp%step(cb, pl, param, outer_time, dto)
-               tp%lfirst = lfirsttp
-            else
-               call tp%step(cb, pl, param, outer_time, dto)
-            end if
-            do j = 1, npl
-               if (pl%nenc(j) == 0) cycle
-               where((tp%plencP(:) == j) .and. (tp%status(:) == INACTIVE)) tp%status(:) = ACTIVE
-            end do
-         end do
-      end associate
+      select type(pl => system%pl)
+      class is (rmvs_pl)
+         select type(tp => system%tp)
+         class is (rmvs_tp)
+            associate(cb => system%cb, npl => pl%nbody, ntp => tp%nbody)
+               dto = dt / NTENC
+               where(tp%plencP(:) == 0)
+                  tp%status(:) = INACTIVE
+               elsewhere  
+                  tp%lperi(:) = .false.
+               end where
+               do outer_index = 1, NTENC
+                  outer_time = t + (outer_index - 1) * dto
+                  call system%set_beg_end(xbeg = pl%outer(outer_index - 1)%x(:, :), &
+                                          vbeg = pl%outer(outer_index - 1)%v(:, :), &
+                                          xend = pl%outer(outer_index    )%x(:, :))
+                  system%rts = RHPSCALE
+                  lencounter = tp%encounter_check(system, dt) 
+                  if (lencounter) then
+                     ! Interpolate planets in inner encounter region
+                     call rmvs_interp_in(system, param, dto, outer_index) 
+                     ! Step through the inner region
+                     call rmvs_step_in(system, param, outer_time, dto)
+                     lfirsttp = tp%lfirst
+                     tp%lfirst = .true.
+                     call tp%step(system, param, outer_time, dto)
+                     tp%lfirst = lfirsttp
+                  else
+                     call tp%step(system, param, outer_time, dto)
+                  end if
+                  do j = 1, npl
+                     if (pl%nenc(j) == 0) cycle
+                     where((tp%plencP(:) == j) .and. (tp%status(:) == INACTIVE)) tp%status(:) = ACTIVE
+                  end do
+               end do
+            end associate
+         end select
+      end select
       return
 
    end subroutine rmvs_step_out
 
-   subroutine rmvs_step_in(pl, cb, tp, param, outer_time, dto)
+   subroutine rmvs_step_in(system, param, outer_time, dto)
       !! author: David A. Minton
       !!
       !! Step active test particles ahead in the inner encounter region
@@ -128,57 +133,63 @@ subroutine rmvs_step_in(pl, cb, tp, param, outer_time, dto)
       !! Adapted from David E. Kaufmann's Swifter routine rmvs_step_in.f90
       implicit none
       ! Arguments
-      class(rmvs_pl),                intent(inout)  :: pl   !! RMVS massive body object
-      class(rmvs_cb),                intent(inout)  :: cb   !! RMVS central body object
-      class(rmvs_tp),                intent(inout)  :: tp   !! RMVS test particle object
-      class(swiftest_parameters), intent(in)     :: param  !! Input collection of parameters parameters 
-      real(DP),                      intent(in)     :: outer_time    !! Current time
-      real(DP),                      intent(in)     :: dto   !! Step size
+      class(rmvs_nbody_system),   intent(inout) :: system     !! RMVS nbody system object
+      class(swiftest_parameters), intent(inout) :: param      !! Current run configuration parameters 
+      real(DP),                   intent(in)    :: outer_time !! Current time
+      real(DP),                   intent(in)    :: dto        !! Outer step size
       ! Internals
-      logical                                        :: lfirsttp
-      integer(I4B)                                   :: i, j, ipleP
-      real(DP)                                       :: dti, inner_time
-      real(DP), dimension(:, :), allocatable         :: xbeg, xend, vbeg
+      logical                                   :: lfirsttp
+      integer(I4B)                              :: i, j, ipleP
+      real(DP)                                  :: dti, inner_time
 
-      associate(npl => pl%nbody, nenc => pl%nenc)
-         dti = dto / NTPHENC
-         allocate(xbeg, mold=pl%xh)
-         allocate(xend, mold=pl%xh)
-         allocate(vbeg, mold=pl%vh)
-         if (param%loblatecb) call pl%obl_acc(cb)
-         call rmvs_make_planetocentric(pl, cb, tp, param)
-         do i = 1, npl
-            if (nenc(i) == 0) cycle
-            associate(cbenci => pl%planetocentric(i)%cb, plenci => pl%planetocentric(i)%pl, &
-                        tpenci => pl%planetocentric(i)%tp)
-               associate(inner_index => tpenci%index)
-                  ! There are inner encounters with this planet...switch to planetocentric coordinates to proceed
-                  tpenci%lfirst = .true.
-                  inner_time = outer_time
-                  call rmvs_peri_tp(tpenci, pl, inner_time, dti, .true., 0, i, param) 
-                  ! 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(:,:)
-                     call tpenci%set_beg_end(xbeg = plenci%inner(inner_index - 1)%x, &
-                                             xend = plenci%inner(inner_index)%x)
-                     call tpenci%step(cbenci, plenci, param, inner_time, dti)
-                     do j = 1, nenc(i)
-                        tpenci%xheliocentric(:, j) = tpenci%xh(:, j) + pl%inner(inner_index)%x(:,i)
-                     end do
-                     inner_time = outer_time + j * dti
-                     call rmvs_peri_tp(tpenci, pl, inner_time, dti, .false., inner_index, i, param) 
-                  end do
-                  where(tpenci%status(:) == ACTIVE) tpenci%status(:) = INACTIVE
-               end associate
+      select type(pl => system%pl)
+      class is (rmvs_pl)
+         select type (tp => system%tp)
+         class is (rmvs_tp)
+            associate(npl => pl%nbody, cb => system%cb)
+               dti = dto / NTPHENC
+               if (param%loblatecb) call pl%obl_acc(cb)
+               call rmvs_make_planetocentric(system, param)
+               do i = 1, npl
+                  if (pl%nenc(i) == 0) cycle
+                  select type(planetocen_system => pl%planetocentric(i))
+                  class is (rmvs_nbody_system)
+                     select type(plenci => planetocen_system%pl)
+                     class is (rmvs_pl)
+                        select type(tpenci => planetocen_system%tp)
+                        class is (rmvs_tp)
+                           associate(inner_index => tpenci%index)
+                              ! There are inner encounters with this planet...switch to planetocentric coordinates to proceed
+                              tpenci%lfirst = .true.
+                              inner_time = outer_time
+                              call rmvs_peri_tp(tpenci, pl, inner_time, dti, .true., 0, i, param) 
+                              ! 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(:,:)
+                                 call planetocen_system%set_beg_end(xbeg = plenci%inner(inner_index - 1)%x, &
+                                                                    xend = plenci%inner(inner_index)%x)
+                                 call tpenci%step(planetocen_system, param, inner_time, dti)
+                                 do j = 1, pl%nenc(i)
+                                    tpenci%xheliocentric(:, j) = tpenci%xh(:, j) + pl%inner(inner_index)%x(:,i)
+                                 end do
+                                 inner_time = outer_time + j * dti
+                                 call rmvs_peri_tp(tpenci, pl, inner_time, dti, .false., inner_index, i, param) 
+                              end do
+                              where(tpenci%status(:) == ACTIVE) tpenci%status(:) = INACTIVE
+                           end associate
+                        end select
+                     end select
+                  end select
+               end do
+               call rmvs_end_planetocentric(system)
             end associate
-         end do
-         call rmvs_end_planetocentric(pl, cb, tp)
-      end associate
+         end select
+      end select
       return
    end subroutine rmvs_step_in
 
-   subroutine rmvs_interp_in(pl, cb, dt, outer_index, param)
+   subroutine rmvs_interp_in(system, param, dt, outer_index)
       !! author: David A. Minton
       !!
       !! Interpolate planet positions between two Keplerian orbits in inner encounter regio
@@ -188,107 +199,109 @@ subroutine rmvs_interp_in(pl, cb, dt, outer_index, param)
       !! Adapted from Hal Levison's Swift routine rmvs3_interp.f
       implicit none
       ! Arguments
-      class(rmvs_pl),                intent(inout) :: pl     !! RMVS test particle object
-      class(rmvs_cb),                intent(inout) :: cb     !! RMVS central body particle type
-      real(DP),                      intent(in)    :: dt     !! Step size
-      integer(I4B),                  intent(in)    :: outer_index !! Outer substep number within current se
-      class(swiftest_parameters), intent(in)    :: param !! Swiftest parameters file
+      class(rmvs_nbody_system),   intent(inout) :: system      !! RMVS test particle object
+      class(swiftest_parameters), intent(in)    :: param       !! Swiftest parameters file
+      real(DP),                   intent(in)    :: dt          !! Step size
+      integer(I4B),               intent(in)    :: outer_index !! Outer substep number within current set
       ! Internals
-      integer(I4B)                    :: i, inner_index
-      real(DP)                        :: frac, dntphenc
-      real(DP), dimension(:,:), allocatable      :: xtmp, vtmp, xh_original
-      real(DP), dimension(:), allocatable         :: msun, dti
-      integer(I4B), dimension(:), allocatable      :: iflag
-
-      associate (npl => pl%nbody)
-         dntphenc = real(NTPHENC, kind=DP)
+      integer(I4B)                              :: i, inner_index
+      real(DP)                                  :: frac, dntphenc
+      real(DP),     dimension(:,:), allocatable :: xtmp, vtmp, xh_original
+      real(DP),     dimension(:),   allocatable :: GMcb, dti
+      integer(I4B), dimension(:),   allocatable :: iflag
 
-         ! 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(:, :)
-
-         allocate(xtmp,mold=pl%xh)
-         allocate(vtmp,mold=pl%vh)
-         allocate(msun(npl))
-         allocate(dti(npl))
-         allocate(iflag(npl))
-         dti(:) = dt / dntphenc
-         msun(:) = cb%Gmass
-         xtmp(:, :) = pl%inner(0)%x(:, :)
-         vtmp(:, :) = pl%inner(0)%v(:, :)
-         if (param%loblatecb) then
-            allocate(xh_original,source=pl%xh)
-            pl%xh(:, :) = xtmp(:, :) ! Temporarily replace heliocentric position with inner substep values to calculate the oblateness terms
-            call pl%obl_acc(cb)
-            pl%inner(0)%aobl(:, :) = pl%aobl(:, :) ! Save the oblateness acceleration on the planet for this substep
-         end if
-
-         do inner_index = 1, NTPHENC - 1
-            call drift_one(msun(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), &
-                                        dti(1:npl), iflag(1:npl))
-            if (any(iflag(1:npl) /= 0)) then
-               do i = 1, npl
-                  if (iflag(i) /=0) then
-                     write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
-                     write(*, *) msun(i), dti(i)
-                     write(*, *) xtmp(:,i)
-                     write(*, *) vtmp(:,i)
-                     write(*, *) " STOPPING "
-                     call util_exit(failure)
-                  end if
-               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(:,:)
-         end do
+      associate (cb => system%cb, npl => system%pl%nbody)
+         select type(pl => system%pl)
+         class is (rmvs_pl)
+            dntphenc = real(NTPHENC, kind=DP)
 
-         xtmp(:,:) = pl%inner(NTPHENC)%x(:, :)
-         vtmp(:,:) = pl%inner(NTPHENC)%v(:, :)
- 
-         do inner_index = NTPHENC - 1, 1, -1
-            call drift_one(msun(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), &
-                                        -dti(1:npl), iflag(1:npl))
-            if (any(iflag(1:npl) /= 0)) then
-               do i = 1, npl
-                  if (iflag(i) /=0) then
-                     write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
-                     write(*, *) msun(i), -dti(i)
-                     write(*, *) xtmp(:,i)
-                     write(*, *) vtmp(:,i)
-                     write(*, *) " STOPPING "
-                     call util_exit(failure)
-                  end if
-               end do
+            ! 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(:, :)
+   
+            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(:, :)
+            if (param%loblatecb) then
+               allocate(xh_original,source=pl%xh)
+               pl%xh(:, :) = xtmp(:, :) ! Temporarily replace heliocentric position with inner substep values to calculate the oblateness terms
+               call pl%obl_acc(cb)
+               pl%inner(0)%aobl(:, :) = pl%aobl(:, :) ! Save the oblateness acceleration on the planet for this substep
             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(:, :)
-
+   
+            do inner_index = 1, NTPHENC - 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), &
+                                          dti(1:npl), iflag(1:npl))
+               if (any(iflag(1:npl) /= 0)) then
+                  do i = 1, npl
+                     if (iflag(i) /=0) then
+                        write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
+                        write(*, *) GMcb(i), dti(i)
+                        write(*, *) xtmp(:,i)
+                        write(*, *) vtmp(:,i)
+                        write(*, *) " STOPPING "
+                        call util_exit(failure)
+                     end if
+                  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(:,:)
+            end do
+   
+            xtmp(:,:) = pl%inner(NTPHENC)%x(:, :)
+            vtmp(:,:) = pl%inner(NTPHENC)%v(:, :)
+   
+            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), &
+                                          vtmp(1,1:npl), vtmp(2,1:npl), vtmp(3,1:npl), &
+                                          -dti(1:npl), iflag(1:npl))
+               if (any(iflag(1:npl) /= 0)) then
+                  do i = 1, npl
+                     if (iflag(i) /=0) then
+                        write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
+                        write(*, *) GMcb(i), -dti(i)
+                        write(*, *) xtmp(:,i)
+                        write(*, *) vtmp(:,i)
+                        write(*, *) " STOPPING "
+                        call util_exit(failure)
+                     end if
+                  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(:, :)
+   
+               if (param%loblatecb) then
+                  pl%xh(:,:) = pl%inner(inner_index)%x(:, :)
+                  call pl%obl_acc(cb)
+                  pl%inner(inner_index)%aobl(:, :) = pl%aobl(:, :) 
+               end if
+            end do
             if (param%loblatecb) then
-               pl%xh(:,:) = pl%inner(inner_index)%x(:, :)
+               ! Calculate the final value of oblateness accelerations at the final inner substep
+               pl%xh(:,:) = pl%inner(NTPHENC)%x(:, :)
                call pl%obl_acc(cb)
-               pl%inner(inner_index)%aobl(:, :) = pl%aobl(:, :) 
+               pl%inner(NTPHENC)%aobl(:, :) = pl%aobl(:, :) 
+               ! Put the planet positions back into place
+               call move_alloc(xh_original, pl%xh)
             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(:, :)
-            call pl%obl_acc(cb)
-            pl%inner(NTPHENC)%aobl(:, :) = pl%aobl(:, :) 
-            ! Put the planet positions back into place
-            call move_alloc(xh_original, pl%xh)
-         end if
+         end select
       end associate
       return
 
    end subroutine rmvs_interp_in
 
-   subroutine rmvs_interp_out(pl, cb, dt, param)
+   subroutine rmvs_interp_out(system, param, dt)
       !! author: David A. Minton
       !!
       !! Interpolate planet positions between two Keplerian orbits in outer encounter region
@@ -298,72 +311,73 @@ subroutine rmvs_interp_out(pl, cb, dt, param)
       !! Adapted from Hal Levison's Swift routine rmvs3_interp.f
       implicit none
       ! Arguments
-      class(rmvs_pl), intent(inout)   :: pl !! RMVS test particle object
-      class(rmvs_cb), intent(inout)   :: cb   !! RMVS central body particle type
-      real(DP), intent(in)            :: dt   !! Step size
+      class(rmvs_nbody_system),   intent(inout) :: system  !! RMVS nbody system object
       class(swiftest_parameters), intent(in)    :: param !! Swiftest parameters file
+      real(DP),                   intent(in)    :: dt   !! Step size
       ! Internals
-      integer(I4B)                    :: i, outer_index
-      real(DP)                        :: frac, dntenc
-      real(DP), dimension(:,:), allocatable       :: xtmp, vtmp
-      real(DP), dimension(:), allocatable         :: msun, dto
-      integer(I4B), dimension(:), allocatable      :: iflag
+      integer(I4B)                              :: i, outer_index
+      real(DP)                                  :: frac, dntenc
+      real(DP),     dimension(:,:), allocatable :: xtmp, vtmp
+      real(DP),     dimension(:),   allocatable :: GMcb, dto
+      integer(I4B), dimension(:),   allocatable :: iflag
 
-   ! executable code
-      dntenc = real(NTENC, DP)
-      associate (npl => pl%nbody)
-         allocate(xtmp, mold = pl%xh)
-         allocate(vtmp, mold = pl%vh)
-         allocate(msun(npl))
-         allocate(dto(npl))
-         allocate(iflag(npl))
-         dto(:) = dt / dntenc
-         msun(:) = cb%Gmass
-         xtmp(:,:) = pl%outer(0)%x(:, :)
-         vtmp(:,:) = pl%outer(0)%v(:, :)
-         do outer_index = 1, NTENC - 1
-            call drift_one(msun(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), &
-                                        dto(1:npl), iflag(1:npl))
+      dntenc = real(NTENC, kind=DP)
+      associate (cb => system%cb, pl => system%pl, npl => system%pl%nbody)
+         select type(pl => system%pl)
+         class is (rmvs_pl)
+            allocate(xtmp, mold = pl%xh)
+            allocate(vtmp, mold = pl%vh)
+            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(:, :)
+            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), &
+                                          dto(1:npl), iflag(1:npl))
 
-            if (any(iflag(1:npl) /= 0)) then
-               do i = 1, npl
-                  if (iflag(i) /= 0) then
-                     write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
-                     write(*, *) msun(i), dto(i)
-                     write(*, *) xtmp(:,i)
-                     write(*, *) vtmp(:,i)
-                     write(*, *) " STOPPING "
-                     call util_exit(FAILURE)
-                  end if
-               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(:,:)
-         end do
-         xtmp(:,:) = pl%outer(NTENC)%x(:, :)
-         vtmp(:,:) = pl%outer(NTENC)%v(:, :)
-         do outer_index = NTENC - 1, 1, -1
-            call drift_one(msun(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), &
-                                        -dto(1:npl), iflag(1:npl))
-            if (any(iflag(1:npl) /= 0)) then
-               do i = 1, npl
-                  if (iflag(i) /= 0) then
-                     write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
-                     write(*, *) msun(i), -dto(i)
-                     write(*, *) xtmp(:,i)
-                     write(*, *) vtmp(:,i)
-                     write(*, *) " STOPPING "
-                     call util_exit(FAILURE)
-                  end if
-               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(:,:)
-         end do
+               if (any(iflag(1:npl) /= 0)) then
+                  do i = 1, npl
+                     if (iflag(i) /= 0) then
+                        write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
+                        write(*, *) GMcb(i), dto(i)
+                        write(*, *) xtmp(:,i)
+                        write(*, *) vtmp(:,i)
+                        write(*, *) " STOPPING "
+                        call util_exit(FAILURE)
+                     end if
+                  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(:,:)
+            end do
+            xtmp(:,:) = pl%outer(NTENC)%x(:, :)
+            vtmp(:,:) = pl%outer(NTENC)%v(:, :)
+            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), &
+                                          -dto(1:npl), iflag(1:npl))
+               if (any(iflag(1:npl) /= 0)) then
+                  do i = 1, npl
+                     if (iflag(i) /= 0) then
+                        write(*, *) " Planet ", pl%name(i), " is lost!!!!!!!!!!"
+                        write(*, *) GMcb(i), -dto(i)
+                        write(*, *) xtmp(:,i)
+                        write(*, *) vtmp(:,i)
+                        write(*, *) " STOPPING "
+                        call util_exit(FAILURE)
+                     end if
+                  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(:,:)
+            end do
+         end select
       end associate
 
       return
@@ -386,7 +400,7 @@ subroutine rmvs_peri_tp(tp, pl, t, dt, lfirst, inner_index, ipleP, param)
       logical,                       intent(in)    :: lfirst    !! Logical flag indicating whether current invocation is the first
       integer(I4B),                  intent(in)    :: inner_index !! Outer substep number within current set
       integer(I4B),                  intent(in)    :: ipleP     !!  index of RMVS planet being closely encountered
-      class(swiftest_parameters), intent(in)    :: param    !! Input collection of  parameters parameters
+      class(swiftest_parameters), intent(in)    :: param    !! Current run configuration parameters
       ! Internals
       integer(I4B)                                 :: i, id1, id2
       real(DP)                                     :: r2, mu, rhill2, vdotr, a, peri, capm, tperi, rpl
@@ -453,7 +467,7 @@ subroutine rmvs_peri_tp(tp, pl, t, dt, lfirst, inner_index, ipleP, param)
 
    end subroutine rmvs_peri_tp
 
-   subroutine rmvs_make_planetocentric(pl, cb, tp, param)
+   subroutine rmvs_make_planetocentric(system, param)
       !! author: David A. Minton
       !!
       !! When encounters are detected, this method will call the interpolation methods for the planets and 
@@ -462,112 +476,135 @@ subroutine rmvs_make_planetocentric(pl, cb, tp, param)
       !!
       implicit none
       ! Arguments
-      class(rmvs_pl),                 intent(inout)  :: pl !! RMVS test particle object
-      class(rmvs_cb),                 intent(inout)  :: cb   !! RMVS central body particle type
-      class(rmvs_tp),                 intent(inout)  :: tp   !! RMVS test particle object
-      class(swiftest_parameters),  intent(in)     :: param !! Input collection of parameters parameters 
+      class(rmvs_nbody_system),   intent(inout) :: system !! RMVS nbody system object
+      class(swiftest_parameters), intent(in)    :: param  !! Current run configuration parameters 
+
       ! Internals
       integer(I4B)                                   :: i, j, inner_index, ipc2hc
       logical, dimension(:), allocatable             :: encmask
 
-      associate(npl => pl%nbody, ntp => tp%nbody, GMpl => pl%Gmass, nenc => pl%nenc)
-         do i = 1, npl
-            if (nenc(i) == 0) cycle 
-            ! There are inner encounters with this planet
-            if (allocated(encmask)) deallocate(encmask)
-            allocate(encmask(ntp))
-            encmask(:) = tp%plencP(:) == i
-
-            ! Create encountering test particle structure
-            allocate(rmvs_tp :: pl%planetocentric(i)%tp)
-            associate(cbenci => pl%planetocentric(i)%cb, &
-                      plenci => pl%planetocentric(i)%pl, &
-                      tpenci => pl%planetocentric(i)%tp)
-               tpenci%lplanetocentric = .true.
-               call tpenci%setup(nenc(i))
-               tpenci%cb_heliocentric = cb
-               tpenci%ipleP = i
-               tpenci%status(:) = ACTIVE
-               tpenci%name(:) = pack(tp%name(:), encmask(:)) 
-               ! Grab all the encountering test particles and convert them to a planetocentric frame
-               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
-               ! 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(plenci%inner(inner_index)%aobl, mold=pl%inner(inner_index)%aobl)
-                  allocate(cbenci%inner(inner_index)%x(NDIM,1))
-                  allocate(cbenci%inner(inner_index)%v(NDIM,1))
-                  allocate(cbenci%inner(inner_index)%aobl(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) 
-                  cbenci%inner(inner_index)%aobl(:,1) = pl%inner(inner_index)%aobl(:, 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)
-                  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)
+      select type(cb => system%cb)
+      class is (rmvs_cb)
+         select type(pl => system%pl)
+         class is (rmvs_pl)
+            select type (tp => system%tp)
+            class is (rmvs_tp)
+               associate (npl => pl%nbody, ntp => tp%nbody)
+                  do i = 1, npl
+                     if (pl%nenc(i) == 0) cycle 
+                     ! There are inner encounters with this planet
+                     if (allocated(encmask)) deallocate(encmask)
+                     allocate(encmask(ntp))
+                     encmask(:) = tp%plencP(:) == i
+                     allocate(rmvs_tp :: pl%planetocentric(i)%tp)
+                     ! Create encountering test particle structure
+                     select type(cbenci => pl%planetocentric(i)%cb)
+                     class is (rmvs_cb)
+                        select type(plenci => pl%planetocentric(i)%pl)
+                        class is (rmvs_pl)
+                           select type(tpenci => pl%planetocentric(i)%tp)
+                           class is (rmvs_tp)
+                              tpenci%lplanetocentric = .true.
+                              call tpenci%setup(pl%nenc(i))
+                              tpenci%cb_heliocentric = cb
+                              tpenci%ipleP = i
+                              tpenci%status(:) = ACTIVE
+                              tpenci%name(:) = pack(tp%name(:), encmask(:)) 
+                              ! Grab all the encountering test particles and convert them to a planetocentric frame
+                              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
+                              ! 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(plenci%inner(inner_index)%aobl, mold=pl%inner(inner_index)%aobl)
+                                 allocate(cbenci%inner(inner_index)%x(NDIM,1))
+                                 allocate(cbenci%inner(inner_index)%v(NDIM,1))
+                                 allocate(cbenci%inner(inner_index)%aobl(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) 
+                                 cbenci%inner(inner_index)%aobl(:,1) =  pl%inner(inner_index)%aobl(:, 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)
+                                 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
+                              call tpenci%set_mu(cbenci)
+                           end select
+                        end select
+                     end select
                   end do
-               end do
-               call tpenci%set_mu(cbenci)
-            end associate
-         end do
-      end associate
+               end associate
+               end select
+            end select
+         end select
       return
-   end subroutine rmvs_make_planetocentric
+      end subroutine rmvs_make_planetocentric
 
-   subroutine rmvs_end_planetocentric(pl, cb, tp)
+   subroutine rmvs_end_planetocentric(system)
       !! author: David A. Minton
       !!
       !! Deallocates all of the encountering particle data structures for next time
       !!
       implicit none
       ! Arguments
-      class(rmvs_pl),                 intent(inout)  :: pl !! RMVS test particle object
-      class(rmvs_cb),                 intent(inout)  :: cb      !!  RMVS central body object
-      class(rmvs_tp),                 intent(inout)  :: tp   !! RMVS test particle object
+      class(rmvs_nbody_system),    intent(inout)  :: system !! RMVS nbody system object
       ! Internals
       integer(I4B) :: i, j, inner_index
       integer(I4B), dimension(:), allocatable :: tpind
       logical, dimension(:), allocatable :: encmask
 
-      associate(nenc => pl%nenc, npl => pl%nbody, ntp => tp%nbody)
-         do i = 1, npl
-            if (nenc(i) == 0) cycle
-            associate(cbenci => pl%planetocentric(i)%cb, &
-                      tpenci => pl%planetocentric(i)%tp, &
-                      plenci => pl%planetocentric(i)%pl)
-               if (allocated(tpind)) deallocate(tpind)
-               allocate(tpind(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:nenc(i))) = tpenci%status(1:nenc(i)) 
-               do j = 1, NDIM
-                  tp%xh(j, tpind(1:nenc(i))) = tpenci%xh(j,1:nenc(i)) + pl%inner(NTPHENC)%x(j, i)
-                  tp%vh(j, tpind(1:nenc(i))) = tpenci%vh(j,1:nenc(i)) + pl%inner(NTPHENC)%v(j, i)
-               end do
-               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) 
-                  deallocate(plenci%inner(inner_index)%aobl)
-               end do
-            end associate
-         end do
-      end associate
+      select type(cb => system%cb)
+      class is (rmvs_cb)
+         select type(pl => system%pl)
+         class is (rmvs_pl)
+            select type (tp => system%tp)
+            class is (rmvs_tp)
+               associate (npl => pl%nbody, ntp => tp%nbody)
+                  do i = 1, npl
+                     if (pl%nenc(i) == 0) cycle
+                     select type(cbenci => pl%planetocentric(i)%cb)
+                     class is (rmvs_cb)
+                        select type(plenci => pl%planetocentric(i)%pl)
+                        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)) 
+                              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
+                              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) 
+                                 deallocate(plenci%inner(inner_index)%aobl)
+                              end do
+                           end select
+                        end select
+                     end select
+                  end do
+               end associate
+            end select
+         end select
+      end select
       return
    end subroutine rmvs_end_planetocentric
    
diff --git a/src/setup/setup.f90 b/src/setup/setup.f90
index 753c3e90c..03fd6f0f0 100644
--- a/src/setup/setup.f90
+++ b/src/setup/setup.f90
@@ -9,7 +9,7 @@ module subroutine setup_construct_system(system, param)
       implicit none
       ! Arguments
       class(swiftest_nbody_system),  allocatable,  intent(inout) :: system     !! Swiftest system object
-      type(swiftest_parameters),                intent(in)    :: param     !! Swiftest parameters parameters
+      type(swiftest_parameters),                   intent(in)    :: param     !! Swiftest parameters
 
       select case(param%integrator)
       case (BS)
@@ -58,13 +58,15 @@ module subroutine setup_construct_system(system, param)
       return
    end subroutine setup_construct_system
 
-   module procedure setup_body
+   module subroutine setup_body(self,n)
       !! author: David A. Minton
       !!
       !! Constructor for base Swiftest particle class. Allocates space for all particles and
       !! initializes all components with a value.
       !! Note: Timing tests indicate that (NDIM, n) is more efficient than (NDIM, n) 
       implicit none
+      class(swiftest_body),         intent(inout) :: self !! Swiftest generic body object
+      integer,                      intent(in)    :: n    !! Number of particles to allocate space for
 
       self%nbody = n
       if (n <= 0) return
@@ -108,14 +110,16 @@ end subroutine setup_construct_system
       self%mu(:)     = 0.0_DP
 
       return
-   end procedure setup_body
+   end subroutine setup_body
 
-   module procedure setup_pl
+   module subroutine setup_pl(self,n)
       !! author: David A. Minton
       !!
       !! Constructor for base Swiftest massive body class. Allocates space for all particles and
       !! initializes all components with a value. 
       implicit none
+      class(swiftest_pl),           intent(inout) :: self !! Swiftest massive body object
+      integer,                      intent(in)    :: n    !! Number of massive bodies to allocate space for
 
       !> 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
@@ -143,14 +147,16 @@ end subroutine setup_construct_system
       self%Q(:) = 0.0_DP
       self%num_comparisons = 0   
       return
-   end procedure setup_pl
+   end subroutine setup_pl
 
-   module procedure setup_tp
+   module subroutine setup_tp(self, n)
       !! author: David A. Minton
       !!
       !! Constructor for base Swiftest test particle particle class. Allocates space for 
       !! all particles and initializes all components with a value. 
       implicit none
+      class(swiftest_tp),           intent(inout) :: self !! Swiftest test particle object
+      integer,                      intent(in)    :: n    !! Number of bodies to allocate space for
 
       !> 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
@@ -166,45 +172,52 @@ end subroutine setup_construct_system
       self%atp(:)    = 0.0_DP
 
       return
-   end procedure setup_tp
+   end subroutine setup_tp
 
-   module procedure setup_set_msys
+   module subroutine setup_set_msys(self)
       !! author: David A. Minton
       !!
       !! Sets the value of msys and the vector mass quantities based on the total mass of the system
+      implicit none
+      class(swiftest_nbody_system),  intent(inout) :: self    !! Swiftest system objec
       self%msys = self%cb%mass + sum(self%pl%mass(1:self%pl%nbody))
 
       return
-   end procedure setup_set_msys
+   end subroutine setup_set_msys
 
-   module procedure setup_set_mu_pl
+   module subroutine setup_set_mu_pl(self, cb)
       !! author: David A. Minton
       !!
       !! Computes G * (M + m) for each massive body
       implicit none
+      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(:)
 
       return
-   end procedure setup_set_mu_pl
+   end subroutine setup_set_mu_pl
 
-   module procedure setup_set_mu_tp
+   module subroutine setup_set_mu_tp(self, cb)
       !! author: David A. Minton
       !!
       !! Converts certain scalar values to arrays so that they can be used in elemental functions
       implicit none
+      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
 
       return
-   end procedure setup_set_mu_tp
+   end subroutine setup_set_mu_tp
 
-   module procedure setup_set_rhill
+   module subroutine setup_set_rhill(self,cb)
       !! author: David A. Minton
       !!
       !! Sets the value of the Hill's radius
       implicit none
-
+      class(swiftest_pl),           intent(inout) :: self !! Swiftest massive body object
+      class(swiftest_cb),           intent(inout) :: cb   !! Swiftest massive body object
 
       if (self%nbody > 0) then
          call self%xv2el(cb) 
@@ -212,13 +225,14 @@ end subroutine setup_construct_system
       end if
 
       return
-   end procedure setup_set_rhill
+   end subroutine setup_set_rhill
 
-   module procedure setup_set_ir3h  
+   module subroutine setup_set_ir3h(self)
       !! author: David A. Minton
       !!
       !! Sets the inverse heliocentric radius term (1/rh**3) for all bodies in a structure
       implicit none
+      class(swiftest_body),         intent(inout) :: self !! Swiftest generic body object
 
       integer(I4B) :: i
       real(DP) :: r2, irh
@@ -233,6 +247,6 @@ end subroutine setup_construct_system
       end if
 
       return
-   end procedure setup_set_ir3h
+   end subroutine setup_set_ir3h
 
 end submodule s_setup
diff --git a/src/user/user_getacch.f90 b/src/user/user_getacch.f90
index 59b922f15..da3d00578 100644
--- a/src/user/user_getacch.f90
+++ b/src/user/user_getacch.f90
@@ -1,7 +1,7 @@
 submodule(swiftest_classes) s_user_getacch
    use swiftest
 contains
-   module subroutine user_getacch_body(self, cb, param, t)
+   module subroutine user_getacch_body(self, system, param, t)
       !! author: David A. Minton
       !!
       !! Add user-supplied heliocentric accelerations to planets
@@ -9,10 +9,10 @@ module subroutine user_getacch_body(self, cb, param, t)
       !! Adapted from David E. Kaufmann's Swifter routine whm_user_getacch.f90
       implicit none
       ! Arguments
-      class(swiftest_body),          intent(inout) :: self   !! Swiftest massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of user parameters parameters
-      real(DP),                      intent(in)    :: t      !! Current time
+      class(swiftest_body),         intent(inout) :: self   !! Swiftest massive body particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! Swiftest nbody_system_object
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of user parameters
+      real(DP),                     intent(in)    :: t      !! Current time
 
       return
    end subroutine user_getacch_body
diff --git a/src/whm/whm_drift.f90 b/src/whm/whm_drift.f90
index d5f915b13..0ac170991 100644
--- a/src/whm/whm_drift.f90
+++ b/src/whm/whm_drift.f90
@@ -1,7 +1,7 @@
 submodule(whm_classes) whm_drift
    use swiftest
 contains
-   module subroutine whm_drift_pl(self, cb, param, dt)
+   module subroutine whm_drift_pl(self, system, param, dt)
       !! author: David A. Minton
       !!
       !! Loop through planets and call Danby drift routine
@@ -11,20 +11,16 @@ module subroutine whm_drift_pl(self, cb, param, dt)
       implicit none
       ! Arguments
       class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structur
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
+      class(swiftest_nbody_system),  intent(inout) :: system !! WHM nbody system object
+      class(swiftest_parameters),    intent(in)    :: param  !! Current run configuration parameters of 
       real(DP),                      intent(in)    :: dt     !! Stepsize
       ! Internals
-      integer(I4B)                                 :: i
-      real(DP)                                     :: energy, vmag2, rmag  !! Variables used in GR calculation
-      integer(I4B), dimension(:), allocatable      :: iflag
-      real(DP), dimension(:), allocatable          :: dtp
+      integer(I4B)                              :: i
+      real(DP)                                  :: energy, vmag2, rmag  !! Variables used in GR calculation
+      integer(I4B), dimension(:), allocatable   :: iflag
+      real(DP), dimension(:), allocatable       :: dtp
 
-      associate(npl    => self%nbody, &
-         xj     => self%xj, &
-         vj     => self%vj, &
-         status => self%status,&
-         mu     => self%muj)
+      associate(pl => self, npl => self%nbody)
 
          if (npl == 0) return
 
@@ -34,24 +30,24 @@ module subroutine whm_drift_pl(self, cb, param, dt)
 
          if (param%lgr) then
             do i = 1,npl
-               rmag = norm2(xj(:, i))
-               vmag2 = dot_product(vj(:, i),  vj(:, i))
-               energy = 0.5_DP * vmag2 - mu(i) / rmag
+               rmag = norm2(pl%xj(:, i))
+               vmag2 = dot_product(pl%vj(:, i), pl%vj(:, i))
+               energy = 0.5_DP * vmag2 - pl%muj(i) / rmag
                dtp(i) = dt * (1.0_DP + 3 * param%inv_c2 * energy)
             end do
          else
             dtp(:) = dt
          end if 
 
-         call drift_one(mu(1:npl), xj(1,1:npl), xj(2,1:npl), xj(3,1:npl), &
-                                   vj(1,1:npl), vj(2,1:npl), vj(3,1:npl), &
+         call drift_one(pl%muj(1:npl), pl%xj(1,1:npl), pl%xj(2,1:npl), pl%xj(3,1:npl), &
+                                   pl%vj(1,1:npl), pl%vj(2,1:npl), pl%vj(3,1:npl), &
                                    dtp(1:npl), iflag(1:npl))
          if (any(iflag(1:npl) /= 0)) then
             do i = 1, npl
                if (iflag(i) /= 0) then
                   write(*, *) " Planet ", self%name(i), " is lost!!!!!!!!!!"
-                  write(*, *) xj(:,i)
-                  write(*, *) vj(:,i)
+                  write(*, *) pl%xj(:,i)
+                  write(*, *) pl%vj(:,i)
                   write(*, *) " stopping "
                   call util_exit(FAILURE)
                end if
@@ -63,7 +59,7 @@ module subroutine whm_drift_pl(self, cb, param, dt)
 
    end subroutine whm_drift_pl
 
-   module subroutine whm_drift_tp(self, cb, param, dt)
+   module subroutine whm_drift_tp(self, system, param, dt)
       !! author: David A. Minton
       !!
       !! Loop through test particles and call Danby drift routine
@@ -73,44 +69,38 @@ module subroutine whm_drift_tp(self, cb, param, dt)
       !! Adapted from David E. Kaufmann's Swifter routine whm_drift_tp.f90
       implicit none
       ! Arguments
-      class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(whm_tp),                intent(inout) :: self   !! WHM test particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! WHM nbody system object
+      class(swiftest_parameters),   intent(in)    :: param !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: dt     !! Stepsize
       ! Internals
-      integer(I4B)                                 :: i   
-      real(DP)                                     :: energy, vmag2, rmag  !! Variables used in GR calculation
-      integer(I4B), dimension(:), allocatable      :: iflag
-      real(DP), dimension(:), allocatable          :: dtp
-
+      integer(I4B)                              :: i   
+      real(DP)                                  :: energy, vmag2, rmag  !! Variables used in GR calculation
+      integer(I4B), dimension(:), allocatable   :: iflag
+      real(DP), dimension(:), allocatable       :: dtp
 
-      associate(ntp    => self%nbody, &
-         xh     => self%xh, &
-         vh     => self%vh, &
-         status => self%status,&
-         mu     => self%mu)
-         
+      associate(tp => self, ntp => self%nbody)
          if (ntp == 0) return
          allocate(iflag(ntp))
          iflag(:) = 0
          allocate(dtp(ntp))
          if (param%lgr) then
-            do i = 1,ntp
-               rmag = norm2(xh(:, i))
-               vmag2 = dot_product(vh(:, i), vh(:, i))
-               energy = 0.5_DP * vmag2 - cb%Gmass / rmag
+            do i = 1, ntp
+               rmag = norm2(tp%xh(:, i))
+               vmag2 = dot_product(tp%vh(:, i), tp%vh(:, i))
+               energy = 0.5_DP * vmag2 - tp%mu(i) / rmag
                dtp(i) = dt * (1.0_DP + 3 * param%inv_c2 * energy)
             end do
          else
             dtp(:) = dt
          end if 
-         do concurrent(i = 1:ntp, status(i) == ACTIVE)
-            call drift_one(mu(i), xh(1,i), xh(2,i), xh(3,i), &
-                                  vh(1,i), vh(2,i), vh(3,i), &
-                                  dtp(i), iflag(i))
+         do concurrent(i = 1:ntp, tp%status(i) == ACTIVE)
+            call drift_one(tp%mu(i), tp%xh(1,i), tp%xh(2,i), tp%xh(3,i), &
+                                     tp%vh(1,i), tp%vh(2,i), tp%vh(3,i), &
+                                     dtp(i), iflag(i))
          end do
          if (any(iflag(1:ntp) /= 0)) then
-            where(iflag(1:ntp) /= 0) status(1:ntp) = DISCARDED_DRIFTERR
+            where(iflag(1:ntp) /= 0) tp%status(1:ntp) = DISCARDED_DRIFTERR
             do i = 1, ntp
                if (iflag(i) /= 0) write(*, *) "Particle ", self%name(i), " lost due to error in Danby drift"
             end do
@@ -118,6 +108,5 @@ module subroutine whm_drift_tp(self, cb, param, dt)
       end associate
 
       return
-
       end subroutine whm_drift_tp
 end submodule whm_drift
diff --git a/src/whm/whm_getacch.f90 b/src/whm/whm_getacch.f90
index 2bfed8d8f..67ecc7487 100644
--- a/src/whm/whm_getacch.f90
+++ b/src/whm/whm_getacch.f90
@@ -1,7 +1,7 @@
 submodule(whm_classes) s_whm_getacch
    use swiftest
 contains
-   module subroutine whm_getacch_pl(self, cb, param, t)
+   module subroutine whm_getacch_pl(self, system, param, t)
       !! author: David A. Minton
       !!
       !! Compute heliocentric accelerations of planets
@@ -10,16 +10,15 @@ module subroutine whm_getacch_pl(self, cb, param, t)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch.f90
       implicit none
       ! Arguments
-      class(whm_pl),                 intent(inout) :: self     !! WHM massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb  !! Swiftest central body particle data structure
-      class(swiftest_parameters), intent(in)    :: param   !! Input collection of 
-      real(DP),                      intent(in)    :: t        !! Current time
+      class(whm_pl),                intent(inout) :: self   !! WHM massive body particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! Swiftest central body particle data structure
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: t       !! Current time
       ! Internals
-      integer(I4B)                                 :: i
-      real(DP), dimension(NDIM)                    :: ah0
+      integer(I4B)                                :: i
+      real(DP), dimension(NDIM)                   :: ah0
 
-      associate(pl => self, npl => self%nbody, j2rp2 => cb%j2rp2, &
-         ah => self%ah, xh => self%xh, xj => self%xj, vh => self%vh, vj => self%vj)
+      associate(cb => system%cb, pl => self, npl => self%nbody)
          if (npl == 0) return
          call pl%set_ir3()
 
@@ -27,19 +26,20 @@ module subroutine whm_getacch_pl(self, cb, param, t)
          do i = 1, npl
             pl%ah(:, i) = ah0(:)
          end do
+
          call whm_getacch_ah1(cb, pl) 
          call whm_getacch_ah2(cb, pl) 
          call whm_getacch_ah3(pl)
 
          if (param%loblatecb) call pl%obl_acc(cb)
-         if (param%lextra_force) call pl%user_getacch(cb, param, t)
-         if (param%lgr) call pl%gr_getacch(cb, param) 
+         if (param%lextra_force) call pl%user_getacch(system, param, t)
+         if (param%lgr) call pl%gr_getacch(param) 
 
       end associate
       return
    end subroutine whm_getacch_pl
 
-   module subroutine whm_getacch_tp(self, cb, pl, param, t, xh)
+   module subroutine whm_getacch_tp(self, system, param, t, xhp)
       !! author: David A. Minton
       !!
       !! Compute heliocentric accelerations of test particles
@@ -48,40 +48,38 @@ module subroutine whm_getacch_tp(self, cb, pl, param, t, xh)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch_tp.f90
       implicit none
       ! Arguments
-      class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Generic Swiftest central body particle data structuree 
-      class(whm_pl),                 intent(inout) :: pl     !! Generic Swiftest massive body particle data structure. 
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP), dimension(:,:),      intent(in)    :: xh     !! Heliocentric positions of planets
+      class(whm_tp),                intent(inout) :: self   !! WHM test particle data structure
+      class(swiftest_nbody_system), intent(inout) :: system !! Swiftest central body particle data structure
+      class(swiftest_parameters),   intent(in)    :: param  !! Current run configuration parameters of 
+      real(DP),                     intent(in)    :: t      !! Current time
+      real(DP), dimension(:,:),     intent(in)    :: xhp    !! Heliocentric positions of planets at the current substep
       ! Internals
-      integer(I4B)                                 :: i
-      real(DP), dimension(NDIM)                    :: ah0
+      integer(I4B)                                :: i
+      real(DP), dimension(NDIM)                   :: ah0
    
-      associate(tp => self, ntp => self%nbody, npl => pl%nbody, j2rp2 => cb%j2rp2, aht => self%ah, &
-               ir3h => pl%ir3h, GMpl => pl%Gmass)
+      associate(tp => self, ntp => self%nbody, pl => system%pl, cb => system%cb, npl => system%pl%nbody)
          if (ntp == 0 .or. npl == 0) return
 
-         ah0 = whm_getacch_ah0(pl%Gmass(:), xh(:,:), npl)
+         ah0(:) = whm_getacch_ah0(pl%Gmass(:), xhp(:,:), npl)
          do i = 1, ntp
             tp%ah(:, i) = ah0(:)
          end do
-         call whm_getacch_ah3_tp(cb, pl, tp, xh)
+         call whm_getacch_ah3_tp(system, xhp)
          if (param%loblatecb) call tp%obl_acc(cb)
-         if (param%lextra_force) call tp%user_getacch(cb, param, t)
-         if (param%lgr) call tp%gr_getacch(cb, param) 
+         if (param%lextra_force) call tp%user_getacch(system, param, t)
+         if (param%lgr) call tp%gr_getacch(param) 
       end associate
       return
    end subroutine whm_getacch_tp
 
-   function whm_getacch_ah0(mu, xh, n) result(ah0)
+   function whm_getacch_ah0(mu, xhp, n) result(ah0)
       !! author: David A. Minton
       !!
       !! Compute zeroth term heliocentric accelerations of planets 
       implicit none
       ! Arguments
       real(DP), dimension(:),   intent(in)         :: mu
-      real(DP), dimension(:,:), intent(in)         :: xh
+      real(DP), dimension(:,:), intent(in)         :: xhp
       integer(I4B),             intent(in)         :: n
       ! Result
       real(DP), dimension(NDIM)                    :: ah0
@@ -91,10 +89,10 @@ function whm_getacch_ah0(mu, xh, n) result(ah0)
 
       ah0(:) = 0.0_DP
       do i = 1, n
-         r2 = dot_product(xh(:, i), xh(:, i))
+         r2 = dot_product(xhp(:, i), xhp(:, i))
          ir3h = 1.0_DP / (r2 * sqrt(r2))
          fac = mu(i) * ir3h 
-         ah0(:) = ah0(:) - fac * xh(:, i)
+         ah0(:) = ah0(:) - fac * xhp(:, i)
       end do
 
       return
@@ -109,17 +107,17 @@ pure subroutine whm_getacch_ah1(cb, pl)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch_ah1.f90
       implicit none
       ! Arguments
-      class(swiftest_cb), intent(in)  :: cb !! Swiftest central body object
-      class(whm_pl), intent(inout)    :: pl !! WHM massive body object
+      class(swiftest_cb), intent(in)    :: cb !! WHM central body object
+      class(whm_pl),      intent(inout) :: pl !! WHM massive body object
       ! Internals
-      integer(I4B)                    :: i
-      real(DP), dimension(NDIM)       :: ah1h, ah1j
+      integer(I4B)                 :: i
+      real(DP), dimension(NDIM)    :: ah1h, ah1j
 
-      associate(npl => pl%nbody, msun => cb%Gmass, xh => pl%xh, xj => pl%xj, ir3j => pl%ir3j, ir3h => pl%ir3h )
+      associate(npl => pl%nbody)
          do i = 2, npl
-            ah1j(:) = xj(:, i) * ir3j(i)
-            ah1h(:) = xh(:, i) * ir3h(i)
-            pl%ah(:, i) = pl%ah(:, i) + msun * (ah1j(:) - ah1h(:))
+            ah1j(:) = pl%xj(:, i) * pl%ir3j(i)
+            ah1h(:) = pl%xh(:, i) * pl%ir3h(i)
+            pl%ah(:, i) = pl%ah(:, i) + cb%Gmass * (ah1j(:) - ah1h(:))
          end do
       end associate
    
@@ -136,21 +134,21 @@ pure subroutine whm_getacch_ah2(cb, pl)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch_ah2.f90
       implicit none
       ! Arguments
-      class(swiftest_cb), intent(in)     :: cb !! Swiftest central body object
-      class(whm_pl),      intent(inout)  :: pl !! WHM massive body object
+      class(swiftest_cb), intent(in)    :: cb !! Swiftest central body object
+      class(whm_pl),      intent(inout) :: pl !! WHM massive body object
       ! Internals
-      integer(I4B)                                 :: i
-      real(DP)                                     :: etaj, fac
-      real(DP), dimension(NDIM)                    :: ah2, ah2o
+      integer(I4B)                 :: i
+      real(DP)                     :: etaj, fac
+      real(DP), dimension(NDIM)    :: ah2, ah2o
    
-      associate(npl => pl%nbody, Gmsun => cb%Gmass, xh => pl%xh, xj => pl%xj, Gmpl => pl%Gmass, ir3j => pl%ir3j)
+      associate(npl => pl%nbody)
          ah2(:) = 0.0_DP
          ah2o(:) = 0.0_DP
-         etaj = Gmsun
+         etaj = cb%Gmass
          do i = 2, npl
-            etaj = etaj + Gmpl(i - 1)
-            fac = Gmpl(i) * Gmsun * ir3j(i) / etaj
-            ah2(:) = ah2o + fac * xj(:, i)
+            etaj = etaj + pl%Gmass(i - 1)
+            fac = pl%Gmass(i) * cb%Gmass * pl%ir3j(i) / etaj
+            ah2(:) = ah2o + fac * pl%xj(:, i)
             pl%ah(:,i) = pl%ah(:, i) + ah2(:)
             ah2o(:) = ah2(:)
          end do
@@ -168,23 +166,23 @@ pure subroutine whm_getacch_ah3(pl)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch_ah3.f90
       implicit none
 
-      class(whm_pl),           intent(inout)       :: pl
-      integer(I4B)                                 :: i, j
-      real(DP)                                     :: rji2, irij3, faci, facj
-      real(DP), dimension(NDIM)                    :: dx
-      real(DP), dimension(:,:), allocatable        :: ah3
+      class(whm_pl),           intent(inout) :: pl
+      integer(I4B)                           :: i, j
+      real(DP)                               :: rji2, irij3, faci, facj
+      real(DP), dimension(NDIM)              :: dx
+      real(DP), dimension(:,:), allocatable  :: ah3
    
-      associate(npl => pl%nbody, xh => pl%xh, Gmpl => pl%Gmass) 
+      associate(npl => pl%nbody)
          allocate(ah3, mold=pl%ah)
-         ah3(:, 1:npl) = 0.0_DP
+         ah3(:, :) = 0.0_DP
 
          do i = 1, npl - 1
             do j = i + 1, npl
-               dx(:) = xh(:, j) - xh(:, i)
+               dx(:) = pl%xh(:, j) - pl%xh(:, i)
                rji2  = dot_product(dx(:), dx(:))
                irij3 = 1.0_DP / (rji2 * sqrt(rji2))
-               faci = Gmpl(i) * irij3
-               facj = Gmpl(j) * irij3
+               faci = pl%Gmass(i) * irij3
+               facj = pl%Gmass(j) * irij3
                ah3(:, i) = ah3(:, i) + facj * dx(:)
                ah3(:, j) = ah3(:, j) - faci * dx(:)
             end do
@@ -198,7 +196,7 @@ pure subroutine whm_getacch_ah3(pl)
       return
    end subroutine whm_getacch_ah3
 
-   pure subroutine whm_getacch_ah3_tp(cb, pl, tp, xh) 
+   pure subroutine whm_getacch_ah3_tp(system, xhp) 
       !! author: David A. Minton
       !!
       !! Compute direct cross (third) term heliocentric accelerations of test particles
@@ -207,27 +205,25 @@ pure subroutine whm_getacch_ah3_tp(cb, pl, tp, xh)
       !! Adapted from David E. Kaufmann's Swifter routine whm_getacch_ah3.f90
       implicit none
       ! Arguments
-      class(swiftest_cb), intent(in)               :: cb  !! Swiftest central body object
-      class(whm_pl), intent(in)                    :: pl  !! WHM massive body object
-      class(whm_tp), intent(inout)                 :: tp  !! WHM test particle object
-      real(DP), dimension(:,:), intent(in)         :: xh  !! Position vector of massive bodies at required point in step
+      class(swiftest_nbody_system),  intent(inout) :: system !! WHM nbody system object
+      real(DP), dimension(:,:),      intent(in)    :: xhp    !! Heliocentric positions of planets at the current substep
       ! Internals
-      integer(I4B)                                 :: i, j
-      real(DP)                                     :: rji2, irij3, fac
-      real(DP), dimension(NDIM)                    :: dx, acc
+      integer(I4B)                         :: i, j
+      real(DP)                             :: rji2, irij3, fac
+      real(DP), dimension(NDIM)            :: dx, acc
 
-      associate(ntp => tp%nbody, npl => pl%nbody, msun => cb%Gmass,  GMpl => pl%Gmass, xht => tp%xh, aht => tp%ah)
+      associate(ntp => system%tp%nbody, npl => system%pl%nbody, tp => system%tp, pl => system%pl) 
          if (ntp == 0) return
          do i = 1, ntp
             acc(:) = 0.0_DP
             do j = 1, npl
-               dx(:) = xht(:, i) - xh(:, j)
+               dx(:) = tp%xh(:, i) - xhp(:, j)
                rji2 = dot_product(dx(:), dx(:))
                irij3 = 1.0_DP / (rji2 * sqrt(rji2))
-               fac = GMpl(j) * irij3
+               fac = pl%Gmass(j) * irij3
                acc(:) = acc(:) - fac * dx(:)
             end do
-            aht(:, i) = aht(:, i) + acc(:)
+            tp%ah(:, i) = tp%ah(:, i) + acc(:)
          end do
       end associate
       return
diff --git a/src/whm/whm_gr.f90 b/src/whm/whm_gr.f90
index e938b0b9b..363ce5ad4 100644
--- a/src/whm/whm_gr.f90
+++ b/src/whm/whm_gr.f90
@@ -1,8 +1,7 @@
 submodule(whm_classes) s_whm_gr
    use swiftest
 contains
-   module subroutine whm_gr_getacch_pl(self, cb, param)
-      !! author: David A. Minton
+   module subroutine whm_gr_getacch_pl(self, param) !! author: David A. Minton
       !!
       !! Compute relativisitic accelerations of massive bodies
       !!    Based on Saha & Tremaine (1994) Eq. 28
@@ -10,20 +9,18 @@ module subroutine whm_gr_getacch_pl(self, cb, param)
       !! Adapted from David A. Minton's Swifter routine routine gr_whm_getacch.f90
       implicit none
       ! Arguments
-      class(whm_pl),       intent(inout)           :: self   !! WHM massive body particle data structure
-      class(swiftest_cb),  intent(inout)           :: cb     !! Swiftest central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
+      class(whm_pl),              intent(inout) :: self   !! WHM massive body particle data structure
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of 
       ! Internals
       integer(I4B)                                 :: i
       real(DP), dimension(NDIM)                    :: suma
       real(DP), dimension(:, :), allocatable       :: aj
       real(DP)                                     :: beta, rjmag4
       
-      associate(n => self%nbody, msun => cb%Gmass, mu => self%muj, c2 => param%inv_c2, &
+      associate(n => self%nbody, mu => self%muj, c2 => param%inv_c2, &
          ah => self%ah, xj => self%xj, GMpl => self%Gmass, eta => self%eta)
          if (n == 0) return
          allocate(aj, mold = ah)
-         !do concurrent(i = 1:n)
          do i = 1, n
             rjmag4 = (dot_product(xj(:, i), xj(:, i)))**2
             beta   = - mu(i)**2 * c2 
@@ -39,7 +36,7 @@ module subroutine whm_gr_getacch_pl(self, cb, param)
       return
    end subroutine whm_gr_getacch_pl
 
-   module subroutine whm_gr_getacch_tp(self, cb, param)
+   module subroutine whm_gr_getacch_tp(self, param)
       !! author: David A. Minton
       !!
       !! Compute relativisitic accelerations of test particles
@@ -48,17 +45,15 @@ module subroutine whm_gr_getacch_tp(self, cb, param)
       !! Adapted from David A. Minton's Swifter routine routine gr_whm_getacch.f90
       implicit none
       ! Arguments
-      class(whm_tp),                 intent(inout) :: self   !! WHM massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structuree
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
+      class(whm_tp),              intent(inout) :: self   !! WHM massive body particle data structure
+      class(swiftest_parameters), intent(in)    :: param  !! Current run configuration parameters 
       ! Internals
       integer(I4B)                                 :: i
       real(DP)                                     :: rjmag4, beta
       
-      associate(n => self%nbody, msun => cb%Gmass, mu => self%mu,& 
+      associate(n => self%nbody, mu => self%mu,& 
          c2 => param%inv_c2, ah => self%ah, xh => self%xh, status => self%status)
          if (n == 0) return
-         !do concurrent (i = 1:n, status(i) == active)
          do i = 1, n
             rjmag4 = (dot_product(xh(:, i), xh(:, i)))**2
             beta = - mu(i)**2 * c2 
@@ -77,15 +72,14 @@ module pure subroutine whm_gr_p4_pl(self, param, dt)
       !! Adapted from David A. Minton's Swifter routine routine gr_whm_p4.f90
       implicit none
       ! Arguments
-      class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
-      real(DP),                      intent(in)    :: dt     !! Step size
+      class(whm_pl),              intent(inout) :: self   !! Swiftest particle object
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
+      real(DP),                   intent(in)    :: dt     !! Step size
       ! Internals
       integer(I4B)                                 :: i
 
       associate(n => self%nbody, xj => self%xj, vj => self%vj, status => self%status, c2 => param%inv_c2)
          if (n == 0) return
-         !do concurrent (i = 1:n, status(i) == ACTIVE)
          do i = 1,n
             call p4_func(xj(:, i), vj(:, i), dt, c2)
          end do
@@ -104,7 +98,7 @@ module pure subroutine whm_gr_p4_tp(self, param, dt)
       implicit none
       ! Arguments
       class(whm_tp),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       real(DP),                      intent(in)    :: dt     !! Step size
       ! Internals
       integer(I4B)                                 :: i
@@ -128,7 +122,7 @@ module pure subroutine whm_gr_pv2vh_pl(self, param)
       implicit none
       ! Arguments
       class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       ! Internals
       integer(I4B)                                 :: i
       real(DP), dimension(:,:), allocatable        :: vh !! Temporary holder of pseudovelocity for in-place conversion
@@ -154,7 +148,7 @@ module pure subroutine whm_gr_pv2vh_tp(self, param)
       implicit none
       ! Arguments
       class(whm_tp),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       ! Internals
       integer(I4B)                                 :: i
       real(DP), dimension(:,:), allocatable        :: vh !! Temporary holder of pseudovelocity for in-place conversion
@@ -180,7 +174,7 @@ module pure subroutine whm_gr_vh2pv_pl(self, param)
       implicit none
       ! Arguments
       class(whm_pl),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       ! Internals
       integer(I4B)                                 :: i
       real(DP), dimension(:,:), allocatable        :: pv !! Temporary holder of pseudovelocity for in-place conversion
@@ -206,7 +200,7 @@ module pure subroutine whm_gr_vh2pv_tp(self, param)
       implicit none
       ! Arguments
       class(whm_tp),                 intent(inout) :: self   !! Swiftest particle object
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of on parameters 
+      class(swiftest_parameters), intent(in)    :: param !! Current run configuration parameters of on parameters 
       ! Internals
       integer(I4B)                                 :: i
       real(DP), dimension(:,:), allocatable        :: pv !! Temporary holder of pseudovelocity for in-place conversion
@@ -234,7 +228,7 @@ pure subroutine gr_vel2pseudovel(param, mu, xh, vh, pv)
       !! Adapted from David A. Minton's Swifter routine gr_vel2pseudovel.f90
       implicit none
 
-      class(swiftest_parameters), intent(in)  :: param !! Input collection of  parameters parameters 
+      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 
@@ -306,7 +300,7 @@ pure subroutine gr_pseudovel2vel(param, mu, xh, pv, vh)
       !!
       !! Adapted from David A. Minton's Swifter routine gr_pseudovel2vel.f90 
       implicit none
-      class(swiftest_parameters), intent(in)  :: param !! Input collection of  parameters parameters 
+      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)  :: pv     !! Pseudovelocity velocity vector - see Saha & Tremain (1994), eq. (32)
diff --git a/src/whm/whm_setup.f90 b/src/whm/whm_setup.f90
index af3f4c774..e0812d00d 100644
--- a/src/whm/whm_setup.f90
+++ b/src/whm/whm_setup.f90
@@ -80,7 +80,7 @@ module subroutine whm_setup_system(self, param)
       implicit none
       ! Arguments
       class(whm_nbody_system),       intent(inout) :: self    !! Swiftest system object
-      class(swiftest_parameters), intent(inout) :: param  !! Input collection of on parameters 
+      class(swiftest_parameters), intent(inout) :: param  !! Current run configuration parameters of on parameters 
       call io_read_initialize_system(self, param)
       ! Make sure that the discard list gets allocated initially
       call self%tp_discards%setup(self%tp%nbody)
@@ -133,7 +133,7 @@ module subroutine whm_setup_set_beg_end(self, xbeg, xend, vbeg)
       !! Sets one or more of the values of xbeg and xend
       implicit none
       ! Arguments
-      class(whm_tp),            intent(inout)           :: self !! Swiftest test particle object
+      class(whm_nbody_system),  intent(inout)           :: self !! WHM nbody system object
       real(DP), dimension(:,:), intent(in),    optional :: xbeg, xend
       real(DP), dimension(:,:), intent(in),    optional :: vbeg ! vbeg is an unused variable to keep this method forward compatible with RMVS
 
diff --git a/src/whm/whm_step.f90 b/src/whm/whm_step.f90
index da504963b..8e87796ea 100644
--- a/src/whm/whm_step.f90
+++ b/src/whm/whm_step.f90
@@ -2,8 +2,7 @@
    use swiftest
 contains
 
-
-   module subroutine whm_step_system(self, param)
+   module subroutine whm_step_system(self, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step massive bodies and and active test particles ahead in heliocentric coordinates
@@ -12,31 +11,24 @@ module subroutine whm_step_system(self, param)
       !! Adapted from David E. Kaufmann's Swifter routine whm_step.f90
       implicit none
       ! Arguments
-      class(whm_nbody_system),      intent(inout) :: self    !! WHM nbody system object
-      class(swiftest_parameters), intent(in)    :: param  !! Input collection of on parameters 
+      class(whm_nbody_system),    intent(inout) :: self  !! WHM nbody system object
+      class(swiftest_parameters), intent(inout) :: param !! Current run configuration parameters of on parameters 
+      real(DP),                   intent(in)    :: t     !! Current simulation time
+      real(DP),                   intent(in)    :: dt    !! Current stepsize
 
-      select type(cb => self%cb)
-      class is (whm_cb)
-      select type(pl => self%pl)
-      class is (whm_pl)
-      select type(tp => self%tp)
-      class is (whm_tp)
-      associate(ntp => tp%nbody, npl => pl%nbody, t => param%t, dt => param%dt)
+      associate(system => self, cb => self%cb,  pl => self%pl, tp => self%tp, ntp => self%tp%nbody, npl => self%pl%nbody)
          call pl%set_rhill(cb)
-         call tp%set_beg_end(xbeg = pl%xh)
-         call pl%step(cb, param, t, dt)
+         call self%set_beg_end(xbeg = pl%xh)
+         call pl%step(system, param, t, dt)
          if (ntp > 0) then
-            call tp%set_beg_end(xend = pl%xh)
-            call tp%step(cb, pl, param, t, dt)
+            call self%set_beg_end(xend = pl%xh)
+            call tp%step(system, param, t, dt)
          end if
       end associate
-      end select
-      end select
-      end select
       return
    end subroutine whm_step_system 
 
-   module subroutine whm_step_pl(self, cb, param, t, dt)
+   module subroutine whm_step_pl(self, system, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step planets ahead using kick-drift-kick algorithm
@@ -46,37 +38,35 @@ module subroutine whm_step_pl(self, cb, param, t, dt)
       !logical, save :: lfirst = .true.
       implicit none
       ! Arguments
-      class(whm_pl),                 intent(inout) :: self   !! WHM massive body particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(whm_pl),                intent(inout) :: self   !! WHM massive body particle data structure
+      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     !! Current simulation time
+      real(DP),                     intent(in)    :: dt    !! Current stepsize
       ! Internals
-      real(DP)                                     :: dth
+      real(DP)                                    :: dth
       
-      associate(pl => self, xh => self%xh, vh => self%vh, ah => self%ah, &
-               xj => self%xj, vj => self%vj)
+      associate(pl => self, cb => system%cb)
          dth = 0.5_DP * dt
          if (pl%lfirst) then
             call pl%h2j(cb)
-            call pl%getacch(cb, param, t)
+            call pl%getacch(system, param, t)
             pl%lfirst = .false.
          end if
-
          call pl%kickvh(dth)
          call pl%vh2vj(cb) 
          !If GR enabled, calculate the p4 term before and after each drift
          if (param%lgr) call pl%gr_p4(param, dth)
-         call pl%drift(cb, param, dt)
+         call pl%drift(system, param, dt)
          if (param%lgr) call pl%gr_p4(param, dth)
          call pl%j2h(cb)
-         call pl%getacch(cb, param, t + dt)
+         call pl%getacch(system, param, t + dt)
          call pl%kickvh(dth)
       end associate
       return
    end subroutine whm_step_pl
 
-   module subroutine whm_step_tp(self, cb, pl, param, t, dt)
+   module subroutine whm_step_tp(self, system, param, t, dt)
       !! author: David A. Minton
       !!
       !! Step active test particles ahead using kick-drift-kick algorithm
@@ -85,30 +75,31 @@ module subroutine whm_step_tp(self, cb, pl, param, t, dt)
       !! Adapted from David E. Kaufmann's Swifter routine whm_step_tp.f90
       implicit none
       ! Arguments
-      class(whm_tp),                 intent(inout) :: self   !! WHM test particle data structure
-      class(swiftest_cb),            intent(inout) :: cb     !! Swiftest central body particle data structure
-      class(whm_pl),                 intent(inout) :: pl     !! WHM massive body data structure
-      class(swiftest_parameters), intent(in)    :: param !! Input collection of 
-      real(DP),                      intent(in)    :: t      !! Current time
-      real(DP),                      intent(in)    :: dt     !! Stepsize
+      class(whm_tp),                intent(inout) :: self   !! WHM test particle data structure
+      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     !! Current simulation time
+      real(DP),                     intent(in)    :: dt    !! Current stepsize
       ! Internals
-      real(DP)                                     :: dth
+      real(DP)                                    :: dth
 
-      associate(tp => self, xht => self%xh, vht => self%vh, aht => self%ah, &
-         xbeg => self%xbeg, xend => self%xend)
-         dth = 0.5_DP * dt
-         if (tp%lfirst) then
-            call tp%getacch(cb, pl, param, t, xbeg)
-            tp%lfirst = .false.
-         end if
-         call tp%kickvh(dth)
-         !If GR enabled, calculate the p4 term before and after each drift
-         if (param%lgr) call tp%gr_p4(param, dth)
-         call tp%drift(cb, param, dt)
-         if (param%lgr) call tp%gr_p4(param, dth)
-         call tp%getacch(cb, pl, param, t + dt, xend)
-         call tp%kickvh(dth)
-      end associate
+      select type(system)
+      class is (whm_nbody_system)
+         associate(tp => self, cb => system%cb, pl => system%pl, xbeg => system%xbeg, xend => system%xend)
+            dth = 0.5_DP * dt
+            if (tp%lfirst) then
+               call tp%getacch(system, param, t, xbeg)
+               tp%lfirst = .false.
+            end if
+            call tp%kickvh(dth)
+            !If GR enabled, calculate the p4 term before and after each drift
+            if (param%lgr) call tp%gr_p4(param, dth)
+            call tp%drift(system, param, dt)
+            if (param%lgr) call tp%gr_p4(param, dth)
+            call tp%getacch(system, param, t + dt, xend)
+            call tp%kickvh(dth)
+         end associate
+      end select
       return
    end subroutine whm_step_tp