pincell_msr_redox.ipynb

{
 "cells": [
  {
   "cell_type": "code",
   "execution_count": 1,
   "id": "8b2785df",
   "metadata": {},
   "outputs": [
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      "[ca-ws:1422728] mca_base_component_repository_open: unable to open mca_accelerator_rocm: libamdhip64.so.6: cannot open shared object file: No such file or directory (ignored)\n"
     ]
    }
   ],
   "source": [
    "%matplotlib inline\n",
    "from math import pi\n",
    "import openmc\n",
    "import openmc.deplete\n",
    "import matplotlib.pyplot as plt\n",
    "import numpy as np\n",
    "import re"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "7834df82",
   "metadata": {},
   "source": [
    "Let's use the same material definition as the existing pincell depletion example "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 9,
   "id": "45acfbc9",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Instantiate some Materials and register the appropriate Nuclides\n",
    "uf4 = openmc.Material(name='UF4')\n",
    "uf4.set_density('g/cm3', 4.5)\n",
    "uf4.add_element('U', 1., enrichment=2.4)\n",
    "uf4.add_element('F', 4.)\n",
    "\n",
    "helium = openmc.Material(name='Helium for gap')\n",
    "helium.set_density('g/cm3', 0.001598)\n",
    "helium.add_element('He', 2.4044e-4)\n",
    "\n",
    "zircaloy = openmc.Material(name='Zircaloy 4')\n",
    "zircaloy.set_density('g/cm3', 6.55)\n",
    "zircaloy.add_element('Sn', 0.014, 'wo')\n",
    "zircaloy.add_element('Fe', 0.00165, 'wo')\n",
    "zircaloy.add_element('Cr', 0.001, 'wo')\n",
    "zircaloy.add_element('Zr', 0.98335, 'wo')\n",
    "\n",
    "borated_water = openmc.Material(name='Borated water')\n",
    "borated_water.set_density('g/cm3', 0.740582)\n",
    "borated_water.add_element('B', 4.0e-5)\n",
    "borated_water.add_element('H', 5.0e-2)\n",
    "borated_water.add_element('O', 2.4e-2)\n",
    "borated_water.add_s_alpha_beta('c_H_in_H2O')\n",
    "\n",
    "# Define overall material\n",
    "material = openmc.Materials([uf4, helium, zircaloy, borated_water])"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "c9774fc9",
   "metadata": {},
   "source": [
    "The geometry definition is going to be slightly different. Firstly, we want to bound the geometry in `z` assigning a pincell height. Secondly, we want to define a cell that contains a universe made of water and helium cells, separated by an interface, which we can initially set at $-59\\ cm$ so that the initial condition of $k_{eff} \\sim 1$ is satisfied. \n",
    "\n",
    "Filling the `msr` cell with a universe is the requirement to set up a geometrical reactivity controller, as we shall see in the `msr_pincell_reactivity_control` notebook.    "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 10,
   "id": "be80a9b7",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Define surfaces\n",
    "width = 1.25984\n",
    "height = 200\n",
    "fuel_or = openmc.ZCylinder(r=0.39218, name='Fuel OR')\n",
    "clad_ir = openmc.ZCylinder(r=0.40005, name='Clad IR')\n",
    "clad_or = openmc.ZCylinder(r=0.45720, name='Clad OR')\n",
    "wat_or = openmc.ZCylinder(r=width/2, name='H2O OR', boundary_type='reflective')\n",
    "# set initial borated water level to -59 cm \n",
    "interface = openmc.ZPlane(z0=-59, name='IF')\n",
    "z_top = openmc.ZPlane(z0=height/2, name='Pin TOP', boundary_type='vacuum')\n",
    "z_bot = openmc.ZPlane(z0=-height/2, name='Pin BOT', boundary_type='vacuum')\n",
    "\n",
    "# Define cells\n",
    "fuel = openmc.Cell(fill=uf4, region=-fuel_or & -z_top & +z_bot)\n",
    "gap = openmc.Cell(fill=helium, region=+fuel_or & -clad_ir & -z_top & +z_bot)\n",
    "clad = openmc.Cell(fill=zircaloy, region=+clad_ir & -clad_or & -z_top & +z_bot)\n",
    "water = openmc.Cell(fill=borated_water, region=+clad_or & -interface )\n",
    "gas = openmc.Cell(fill=helium, region=+clad_or & +interface)\n",
    "msr_uni = openmc.Universe(cells=(water, gas))\n",
    "msr = openmc.Cell(name=\"MSR\", fill=msr_uni, region=-wat_or & -z_top & +z_bot)\n",
    "root = openmc.Universe(cells=[fuel, gap, clad, msr])\n",
    "# Define overall geometry\n",
    "geometry = openmc.Geometry(root)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 11,
   "id": "ffb4a60e",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Instantiate a Settings object, set all runtime parameters, and export to XML\n",
    "settings = openmc.Settings()\n",
    "settings.batches = 100\n",
    "settings.inactive = 10\n",
    "settings.particles = 1000\n",
    "\n",
    "# Create an initial uniform spatial source distribution over fissionable zones\n",
    "bounds = [-0.62992, -0.62992, -100, 0.62992, 0.62992, 100]\n",
    "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n",
    "settings.source = openmc.source.IndependentSource(space=uniform_dist)\n",
    "\n",
    "#Build the model\n",
    "model = openmc.Model(geometry=geometry, materials=material, settings=settings)"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "df6f8a90",
   "metadata": {},
   "source": [
    "Let's plot the pincell. We can notice the initial interface between the borated water and helium cells."
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 12,
   "id": "be46b587",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/plain": [
       "<Axes: xlabel='x [cm]', ylabel='z [cm]'>"
      ]
     },
     "execution_count": 12,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 258.065x259.74 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "# Create plot\n",
    "colors = {uf4:'red', helium:'cyan', borated_water: 'blue', zircaloy: 'gray'}\n",
    "root.plot(width=(5, 5), origin=(0,0,-59), pixels=(200, 200), basis='xz', color_by='material', colors=colors, legend=True)"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "ec29ddf6",
   "metadata": {},
   "source": [
    "Let's now build and run a standard depletion calculation, increasing the thermal power to $100\\ kW$. The results will be used as the reference to compare with MSR capabilities:"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 13,
   "id": "ac103e03",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "                                %%%%%%%%%%%%%%%\n",
      "                           %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                        %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                      %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                    %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                    %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                     %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                 ###############      %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ##################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ###################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ####################     %%%%%%%%%%%%%%%%%%%%%%\n",
      "                #####################     %%%%%%%%%%%%%%%%%%%%%\n",
      "                ######################     %%%%%%%%%%%%%%%%%%%%\n",
      "                #######################     %%%%%%%%%%%%%%%%%%\n",
      "                 #######################     %%%%%%%%%%%%%%%%%\n",
      "                 ######################     %%%%%%%%%%%%%%%%%\n",
      "                  ####################     %%%%%%%%%%%%%%%%%\n",
      "                    #################     %%%%%%%%%%%%%%%%%\n",
      "                     ###############     %%%%%%%%%%%%%%%%\n",
      "                       ############     %%%%%%%%%%%%%%%\n",
      "                          ########     %%%%%%%%%%%%%%\n",
      "                                      %%%%%%%%%%%\n",
      "\n",
      "                 | The OpenMC Monte Carlo Code\n",
      "       Copyright | 2011-2024 MIT, UChicago Argonne LLC, and contributors\n",
      "         License | https://docs.openmc.org/en/latest/license.html\n",
      "         Version | 0.14.1-dev\n",
      "        Git SHA1 | d93ac83697e7fdb4fd4cc0f2705795398bf804bd\n",
      "       Date/Time | 2024-04-18 15:24:22\n",
      "   MPI Processes | 1\n",
      "  OpenMP Threads | 56\n",
      "\n",
      " Reading settings XML file...\n",
      " Reading cross sections XML file...\n",
      " Reading materials XML file...\n",
      " Reading geometry XML file...\n",
      " Reading U234 from /home/lorenzo/nuclear_data/endfb80_hdf5/U234.h5\n",
      " Reading U235 from /home/lorenzo/nuclear_data/endfb80_hdf5/U235.h5\n",
      " Reading U238 from /home/lorenzo/nuclear_data/endfb80_hdf5/U238.h5\n",
      " Reading F19 from /home/lorenzo/nuclear_data/endfb80_hdf5/F19.h5\n",
      " Reading U236 from /home/lorenzo/nuclear_data/endfb80_hdf5/U236.h5\n",
      " Reading He3 from /home/lorenzo/nuclear_data/endfb80_hdf5/He3.h5\n",
      " Reading He4 from /home/lorenzo/nuclear_data/endfb80_hdf5/He4.h5\n",
      " Reading Cr50 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr50.h5\n",
      " Reading Cr52 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr52.h5\n",
      " Reading Cr53 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr53.h5\n",
      " Reading Cr54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr54.h5\n",
      " Reading Fe54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe54.h5\n",
      " Reading Fe56 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe56.h5\n",
      " Reading Fe57 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe57.h5\n",
      " Reading Fe58 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe58.h5\n",
      " Reading Sn112 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn112.h5\n",
      " Reading Sn114 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn114.h5\n",
      " Reading Sn115 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn115.h5\n",
      " Reading Sn116 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn116.h5\n",
      " Reading Sn117 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn117.h5\n",
      " Reading Sn118 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn118.h5\n",
      " Reading Sn119 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn119.h5\n",
      " Reading Sn120 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn120.h5\n",
      " Reading Sn122 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn122.h5\n",
      " Reading Sn124 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn124.h5\n",
      " Reading Zr90 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr90.h5\n",
      " Reading Zr91 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr91.h5\n",
      " Reading Zr92 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr92.h5\n",
      " Reading Zr94 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr94.h5\n",
      " Reading Zr96 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr96.h5\n",
      " Reading B10 from /home/lorenzo/nuclear_data/endfb80_hdf5/B10.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Negative value(s) found on probability table for nuclide Zr96 at 294K\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading B11 from /home/lorenzo/nuclear_data/endfb80_hdf5/B11.h5\n",
      " Reading H1 from /home/lorenzo/nuclear_data/endfb80_hdf5/H1.h5\n",
      " Reading H2 from /home/lorenzo/nuclear_data/endfb80_hdf5/H2.h5\n",
      " Reading O16 from /home/lorenzo/nuclear_data/endfb80_hdf5/O16.h5\n",
      " Reading O17 from /home/lorenzo/nuclear_data/endfb80_hdf5/O17.h5\n",
      " Reading O18 from /home/lorenzo/nuclear_data/endfb80_hdf5/O18.h5\n",
      " Reading c_H_in_H2O from /home/lorenzo/nuclear_data/endfb80_hdf5/c_H_in_H2O.h5\n",
      " Minimum neutron data temperature: 0 K\n",
      " Maximum neutron data temperature: 1.7976931348623157e+308 K\n",
      " Reading tallies XML file...\n",
      " Preparing distributed cell instances...\n",
      " Reading plot XML file...\n",
      " Writing summary.h5 file...\n",
      "[openmc.deplete] t=0.0 s, dt=86400.0 s, source=100000.0\n",
      " Reading I135 from /home/lorenzo/nuclear_data/endfb80_hdf5/I135.h5\n",
      " Reading Xe135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe135.h5\n",
      " Reading Xe136 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe136.h5\n",
      " Reading Cs135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cs135.h5\n",
      " Reading Gd157 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd157.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Could not find material 5 specified in plot 1\n",
      " WARNING: Could not find material 6 specified in plot 1\n",
      " WARNING: Could not find material 7 specified in plot 1\n",
      " WARNING: Could not find material 8 specified in plot 1\n",
      " WARNING: Could not find material 9 specified in plot 1\n",
      " WARNING: Could not find material 10 specified in plot 1\n",
      " WARNING: Could not find material 5 specified in plot 2\n",
      " WARNING: Could not find material 6 specified in plot 2\n",
      " WARNING: Could not find material 7 specified in plot 2\n",
      " WARNING: Could not find material 8 specified in plot 2\n",
      " WARNING: Could not find material 9 specified in plot 2\n",
      " WARNING: Could not find material 10 specified in plot 2\n",
      " WARNING: Could not find material 5 specified in plot 3\n",
      " WARNING: Could not find material 6 specified in plot 3\n",
      " WARNING: Could not find material 7 specified in plot 3\n",
      " WARNING: Could not find material 8 specified in plot 3\n",
      " WARNING: Could not find material 9 specified in plot 3\n",
      " WARNING: Could not find material 10 specified in plot 3\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading Gd156 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd156.h5\n",
      " Reading Pu239 from /home/lorenzo/nuclear_data/endfb80_hdf5/Pu239.h5\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.55230\n",
      "        2/1    0.71581\n",
      "        3/1    0.84742\n",
      "        4/1    0.82083\n",
      "        5/1    0.88937\n",
      "        6/1    0.83661\n",
      "        7/1    0.90388\n",
      "        8/1    0.89892\n",
      "        9/1    0.84564\n",
      "       10/1    0.89387\n",
      "       11/1    0.81112\n",
      "       12/1    0.90903    0.86007 +/- 0.04896\n",
      "       13/1    0.82243    0.84752 +/- 0.03093\n",
      "       14/1    0.87888    0.85536 +/- 0.02323\n",
      "       15/1    0.85114    0.85452 +/- 0.01801\n",
      "       16/1    0.88721    0.85997 +/- 0.01569\n",
      "       17/1    0.88177    0.86308 +/- 0.01362\n",
      "       18/1    0.90888    0.86881 +/- 0.01311\n",
      "       19/1    0.83572    0.86513 +/- 0.01213\n",
      "       20/1    0.83936    0.86255 +/- 0.01115\n",
      "       21/1    0.94591    0.87013 +/- 0.01262\n",
      "       22/1    0.84293    0.86787 +/- 0.01174\n",
      "       23/1    0.88706    0.86934 +/- 0.01090\n",
      "       24/1    0.87462    0.86972 +/- 0.01010\n",
      "       25/1    0.77153    0.86317 +/- 0.01145\n",
      "       26/1    0.85637    0.86275 +/- 0.01072\n",
      "       27/1    0.80862    0.85956 +/- 0.01056\n",
      "       28/1    0.85113    0.85909 +/- 0.00997\n",
      "       29/1    0.83268    0.85770 +/- 0.00953\n",
      "       30/1    0.86520    0.85808 +/- 0.00905\n",
      "       31/1    0.93140    0.86157 +/- 0.00929\n",
      "       32/1    0.88934    0.86283 +/- 0.00895\n",
      "       33/1    0.87335    0.86329 +/- 0.00856\n",
      "       34/1    0.87573    0.86381 +/- 0.00821\n",
      "       35/1    0.91501    0.86586 +/- 0.00814\n",
      "       36/1    0.82385    0.86424 +/- 0.00799\n",
      "       37/1    0.82322    0.86272 +/- 0.00783\n",
      "       38/1    0.87062    0.86300 +/- 0.00755\n",
      "       39/1    0.86394    0.86304 +/- 0.00729\n",
      "       40/1    0.88725    0.86384 +/- 0.00709\n",
      "       41/1    0.88834    0.86463 +/- 0.00690\n",
      "       42/1    0.85313    0.86427 +/- 0.00669\n",
      "       43/1    0.93063    0.86629 +/- 0.00679\n",
      "       44/1    0.81729    0.86484 +/- 0.00674\n",
      "       45/1    0.79035    0.86272 +/- 0.00689\n",
      "       46/1    0.96206    0.86548 +/- 0.00724\n",
      "       47/1    0.88932    0.86612 +/- 0.00707\n",
      "       48/1    0.93670    0.86798 +/- 0.00713\n",
      "       49/1    0.88749    0.86848 +/- 0.00696\n",
      "       50/1    0.88210    0.86882 +/- 0.00679\n",
      "       51/1    0.83792    0.86806 +/- 0.00667\n",
      "       52/1    0.86035    0.86788 +/- 0.00651\n",
      "       53/1    0.83267    0.86706 +/- 0.00641\n",
      "       54/1    0.86629    0.86704 +/- 0.00626\n",
      "       55/1    0.83651    0.86637 +/- 0.00616\n",
      "       56/1    0.86899    0.86642 +/- 0.00602\n",
      "       57/1    0.86755    0.86645 +/- 0.00589\n",
      "       58/1    0.86296    0.86637 +/- 0.00577\n",
      "       59/1    0.90701    0.86720 +/- 0.00571\n",
      "       60/1    0.88598    0.86758 +/- 0.00561\n",
      "       61/1    0.83798    0.86700 +/- 0.00553\n",
      "       62/1    0.81695    0.86604 +/- 0.00551\n",
      "       63/1    0.90488    0.86677 +/- 0.00545\n",
      "       64/1    0.91599    0.86768 +/- 0.00543\n",
      "       65/1    0.85986    0.86754 +/- 0.00533\n",
      "       66/1    0.85999    0.86740 +/- 0.00523\n",
      "       67/1    0.88330    0.86768 +/- 0.00515\n",
      "       68/1    0.84368    0.86727 +/- 0.00508\n",
      "       69/1    0.86791    0.86728 +/- 0.00499\n",
      "       70/1    0.81372    0.86639 +/- 0.00499\n",
      "       71/1    0.87471    0.86652 +/- 0.00490\n",
      "       72/1    0.82349    0.86583 +/- 0.00487\n",
      "       73/1    0.92667    0.86679 +/- 0.00489\n",
      "       74/1    0.85169    0.86656 +/- 0.00482\n",
      "       75/1    0.83902    0.86614 +/- 0.00477\n",
      "       76/1    0.89600    0.86659 +/- 0.00471\n",
      "       77/1    0.86706    0.86659 +/- 0.00464\n",
      "       78/1    0.84111    0.86622 +/- 0.00459\n",
      "       79/1    0.80299    0.86530 +/- 0.00462\n",
      "       80/1    0.86359    0.86528 +/- 0.00455\n",
      "       81/1    0.80849    0.86448 +/- 0.00456\n",
      "       82/1    0.89804    0.86495 +/- 0.00452\n",
      "       83/1    0.86185    0.86490 +/- 0.00445\n",
      "       84/1    0.86501    0.86490 +/- 0.00439\n",
      "       85/1    0.84290    0.86461 +/- 0.00434\n",
      "       86/1    0.88679    0.86490 +/- 0.00430\n",
      "       87/1    0.92261    0.86565 +/- 0.00431\n",
      "       88/1    0.82757    0.86516 +/- 0.00428\n",
      "       89/1    0.87889    0.86534 +/- 0.00423\n",
      "       90/1    0.88855    0.86563 +/- 0.00418\n",
      "       91/1    0.85702    0.86552 +/- 0.00413\n",
      "       92/1    0.86806    0.86555 +/- 0.00408\n",
      "       93/1    0.88195    0.86575 +/- 0.00404\n",
      "       94/1    0.86865    0.86578 +/- 0.00399\n",
      "       95/1    0.89434    0.86612 +/- 0.00396\n",
      "       96/1    0.93531    0.86693 +/- 0.00399\n",
      "       97/1    0.91389    0.86747 +/- 0.00398\n",
      "       98/1    0.88900    0.86771 +/- 0.00395\n",
      "       99/1    0.86813    0.86771 +/- 0.00390\n",
      "      100/1    0.84827    0.86750 +/- 0.00386\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 3.2607e+00 seconds\n",
      "   Reading cross sections          = 3.2360e+00 seconds\n",
      " Total time in simulation          = 7.7145e+00 seconds\n",
      "   Time in transport only          = 7.4784e+00 seconds\n",
      "   Time in inactive batches        = 2.6246e-01 seconds\n",
      "   Time in active batches          = 7.4521e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0879e-02 seconds\n",
      "     Sampling source sites         = 9.0295e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5101e-03 seconds\n",
      "   Time accumulating tallies       = 2.0746e-01 seconds\n",
      "   Time writing statepoints        = 7.8764e-03 seconds\n",
      " Total time for finalization       = 1.5423e-04 seconds\n",
      " Total time elapsed                = 1.1002e+01 seconds\n",
      " Calculation Rate (inactive)       = 38101.8 particles/second\n",
      " Calculation Rate (active)         = 12077.2 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.87058 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.86750 +/- 0.00386\n",
      " k-effective (Absorption)    = 0.88032 +/- 0.00359\n",
      " Combined k-effective        = 0.87426 +/- 0.00317\n",
      " Leakage Fraction            = 0.13803 +/- 0.00134\n",
      "\n",
      " Creating state point openmc_simulation_n0.h5...\n",
      "[openmc.deplete] t=86400.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50806\n",
      "        2/1    0.63230\n",
      "        3/1    0.69701\n",
      "        4/1    0.81079\n",
      "        5/1    0.93274\n",
      "        6/1    0.83321\n",
      "        7/1    0.96314\n",
      "        8/1    0.94912\n",
      "        9/1    0.90540\n",
      "       10/1    0.86956\n",
      "       11/1    0.83414\n",
      "       12/1    0.84054    0.83734 +/- 0.00320\n",
      "       13/1    0.87119    0.84862 +/- 0.01143\n",
      "       14/1    0.89834    0.86105 +/- 0.01483\n",
      "       15/1    0.81754    0.85235 +/- 0.01441\n",
      "       16/1    0.86838    0.85502 +/- 0.01207\n",
      "       17/1    0.87626    0.85806 +/- 0.01064\n",
      "       18/1    0.81934    0.85322 +/- 0.01041\n",
      "       19/1    0.88481    0.85673 +/- 0.00983\n",
      "       20/1    0.86465    0.85752 +/- 0.00883\n",
      "       21/1    0.93744    0.86478 +/- 0.01079\n",
      "       22/1    0.86246    0.86459 +/- 0.00986\n",
      "       23/1    0.83949    0.86266 +/- 0.00927\n",
      "       24/1    0.93370    0.86773 +/- 0.00997\n",
      "       25/1    0.87229    0.86804 +/- 0.00929\n",
      "       26/1    0.81609    0.86479 +/- 0.00927\n",
      "       27/1    0.85221    0.86405 +/- 0.00874\n",
      "       28/1    0.86951    0.86435 +/- 0.00825\n",
      "       29/1    0.87150    0.86473 +/- 0.00781\n",
      "       30/1    0.88973    0.86598 +/- 0.00751\n",
      "       31/1    0.84004    0.86474 +/- 0.00725\n",
      "       32/1    0.84717    0.86395 +/- 0.00696\n",
      "       33/1    0.90349    0.86567 +/- 0.00687\n",
      "       34/1    0.85706    0.86531 +/- 0.00659\n",
      "       35/1    0.87759    0.86580 +/- 0.00634\n",
      "       36/1    0.87653    0.86621 +/- 0.00610\n",
      "       37/1    0.85567    0.86582 +/- 0.00589\n",
      "       38/1    0.87052    0.86599 +/- 0.00567\n",
      "       39/1    0.88793    0.86674 +/- 0.00553\n",
      "       40/1    0.85401    0.86632 +/- 0.00536\n",
      "       41/1    0.84051    0.86549 +/- 0.00525\n",
      "       42/1    0.79537    0.86330 +/- 0.00553\n",
      "       43/1    0.85048    0.86291 +/- 0.00538\n",
      "       44/1    0.84347    0.86234 +/- 0.00525\n",
      "       45/1    0.90915    0.86367 +/- 0.00527\n",
      "       46/1    0.82163    0.86251 +/- 0.00525\n",
      "       47/1    0.91525    0.86393 +/- 0.00530\n",
      "       48/1    0.81870    0.86274 +/- 0.00530\n",
      "       49/1    0.85609    0.86257 +/- 0.00516\n",
      "       50/1    0.90621    0.86366 +/- 0.00515\n",
      "       51/1    0.85370    0.86342 +/- 0.00503\n",
      "       52/1    0.84083    0.86288 +/- 0.00494\n",
      "       53/1    0.89194    0.86356 +/- 0.00487\n",
      "       54/1    0.85535    0.86337 +/- 0.00476\n",
      "       55/1    0.84042    0.86286 +/- 0.00468\n",
      "       56/1    0.84515    0.86248 +/- 0.00459\n",
      "       57/1    0.86674    0.86257 +/- 0.00449\n",
      "       58/1    0.85369    0.86238 +/- 0.00440\n",
      "       59/1    0.88565    0.86286 +/- 0.00434\n",
      "       60/1    0.82471    0.86209 +/- 0.00432\n",
      "       61/1    0.89567    0.86275 +/- 0.00428\n",
      "       62/1    0.88301    0.86314 +/- 0.00422\n",
      "       63/1    0.80540    0.86205 +/- 0.00428\n",
      "       64/1    0.86508    0.86211 +/- 0.00420\n",
      "       65/1    0.91138    0.86300 +/- 0.00422\n",
      "       66/1    0.84687    0.86272 +/- 0.00415\n",
      "       67/1    0.84292    0.86237 +/- 0.00409\n",
      "       68/1    0.84375    0.86205 +/- 0.00404\n",
      "       69/1    0.83812    0.86164 +/- 0.00399\n",
      "       70/1    0.84045    0.86129 +/- 0.00394\n",
      "       71/1    0.88418    0.86166 +/- 0.00389\n",
      "       72/1    0.84079    0.86133 +/- 0.00384\n",
      "       73/1    0.91448    0.86217 +/- 0.00387\n",
      "       74/1    0.83281    0.86171 +/- 0.00384\n",
      "       75/1    0.90642    0.86240 +/- 0.00384\n",
      "       76/1    0.85093    0.86223 +/- 0.00379\n",
      "       77/1    0.82462    0.86166 +/- 0.00377\n",
      "       78/1    0.91095    0.86239 +/- 0.00379\n",
      "       79/1    0.88209    0.86268 +/- 0.00374\n",
      "       80/1    0.81184    0.86195 +/- 0.00376\n",
      "       81/1    0.86221    0.86195 +/- 0.00371\n",
      "       82/1    0.92138    0.86278 +/- 0.00375\n",
      "       83/1    0.80252    0.86195 +/- 0.00379\n",
      "       84/1    0.85711    0.86189 +/- 0.00373\n",
      "       85/1    0.90975    0.86253 +/- 0.00374\n",
      "       86/1    0.90208    0.86305 +/- 0.00373\n",
      "       87/1    0.90329    0.86357 +/- 0.00371\n",
      "       88/1    0.85103    0.86341 +/- 0.00367\n",
      "       89/1    0.82958    0.86298 +/- 0.00365\n",
      "       90/1    0.90505    0.86351 +/- 0.00364\n",
      "       91/1    0.89412    0.86388 +/- 0.00362\n",
      "       92/1    0.85387    0.86376 +/- 0.00357\n",
      "       93/1    0.88736    0.86405 +/- 0.00354\n",
      "       94/1    0.81615    0.86348 +/- 0.00354\n",
      "       95/1    0.86475    0.86349 +/- 0.00350\n",
      "       96/1    0.85069    0.86334 +/- 0.00347\n",
      "       97/1    0.89034    0.86365 +/- 0.00344\n",
      "       98/1    0.84930    0.86349 +/- 0.00340\n",
      "       99/1    0.86752    0.86353 +/- 0.00337\n",
      "      100/1    0.81820    0.86303 +/- 0.00337\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.3772e+00 seconds\n",
      "   Time in transport only          = 7.2097e+00 seconds\n",
      "   Time in inactive batches        = 2.5467e-01 seconds\n",
      "   Time in active batches          = 7.1226e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1195e-02 seconds\n",
      "     Sampling source sites         = 9.3394e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5010e-03 seconds\n",
      "   Time accumulating tallies       = 1.3919e-01 seconds\n",
      "   Time writing statepoints        = 7.1492e-03 seconds\n",
      " Total time for finalization       = 1.3221e-04 seconds\n",
      " Total time elapsed                = 7.4060e+00 seconds\n",
      " Calculation Rate (inactive)       = 39265.9 particles/second\n",
      " Calculation Rate (active)         = 12635.9 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86066 +/- 0.00291\n",
      " k-effective (Track-length)  = 0.86303 +/- 0.00337\n",
      " k-effective (Absorption)    = 0.85843 +/- 0.00310\n",
      " Combined k-effective        = 0.86017 +/- 0.00232\n",
      " Leakage Fraction            = 0.14009 +/- 0.00129\n",
      "\n",
      " Creating state point openmc_simulation_n1.h5...\n",
      "[openmc.deplete] t=172800.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50000\n",
      "        2/1    0.67230\n",
      "        3/1    0.81333\n",
      "        4/1    0.83116\n",
      "        5/1    0.84603\n",
      "        6/1    0.82412\n",
      "        7/1    0.83696\n",
      "        8/1    0.80864\n",
      "        9/1    0.83710\n",
      "       10/1    0.81911\n",
      "       11/1    0.84603\n",
      "       12/1    0.80245    0.82424 +/- 0.02179\n",
      "       13/1    0.85435    0.83428 +/- 0.01609\n",
      "       14/1    0.87757    0.84510 +/- 0.01570\n",
      "       15/1    0.81854    0.83979 +/- 0.01327\n",
      "       16/1    0.88028    0.84654 +/- 0.01277\n",
      "       17/1    0.83755    0.84525 +/- 0.01087\n",
      "       18/1    0.85025    0.84588 +/- 0.00943\n",
      "       19/1    0.82337    0.84338 +/- 0.00869\n",
      "       20/1    0.85897    0.84494 +/- 0.00792\n",
      "       21/1    0.81365    0.84209 +/- 0.00771\n",
      "       22/1    0.90952    0.84771 +/- 0.00901\n",
      "       23/1    0.86675    0.84918 +/- 0.00841\n",
      "       24/1    0.84361    0.84878 +/- 0.00780\n",
      "       25/1    0.83803    0.84806 +/- 0.00730\n",
      "       26/1    0.88247    0.85021 +/- 0.00716\n",
      "       27/1    0.85534    0.85051 +/- 0.00673\n",
      "       28/1    0.83554    0.84968 +/- 0.00640\n",
      "       29/1    0.87693    0.85112 +/- 0.00622\n",
      "       30/1    0.90068    0.85359 +/- 0.00640\n",
      "       31/1    0.90216    0.85591 +/- 0.00651\n",
      "       32/1    0.84618    0.85546 +/- 0.00622\n",
      "       33/1    0.93315    0.85884 +/- 0.00684\n",
      "       34/1    0.84767    0.85838 +/- 0.00657\n",
      "       35/1    0.80403    0.85620 +/- 0.00666\n",
      "       36/1    0.85647    0.85621 +/- 0.00640\n",
      "       37/1    0.86092    0.85639 +/- 0.00616\n",
      "       38/1    0.87483    0.85705 +/- 0.00597\n",
      "       39/1    0.85094    0.85684 +/- 0.00577\n",
      "       40/1    0.84368    0.85640 +/- 0.00559\n",
      "       41/1    0.83534    0.85572 +/- 0.00545\n",
      "       42/1    0.89596    0.85698 +/- 0.00542\n",
      "       43/1    0.80237    0.85532 +/- 0.00551\n",
      "       44/1    0.84478    0.85501 +/- 0.00536\n",
      "       45/1    0.88263    0.85580 +/- 0.00526\n",
      "       46/1    0.84709    0.85556 +/- 0.00512\n",
      "       47/1    0.86463    0.85580 +/- 0.00498\n",
      "       48/1    0.88020    0.85645 +/- 0.00489\n",
      "       49/1    0.82771    0.85571 +/- 0.00482\n",
      "       50/1    0.91407    0.85717 +/- 0.00492\n",
      "       51/1    0.91321    0.85853 +/- 0.00499\n",
      "       52/1    0.85098    0.85835 +/- 0.00487\n",
      "       53/1    0.85909    0.85837 +/- 0.00476\n",
      "       54/1    0.85456    0.85828 +/- 0.00465\n",
      "       55/1    0.86662    0.85847 +/- 0.00455\n",
      "       56/1    0.79767    0.85715 +/- 0.00464\n",
      "       57/1    0.81819    0.85632 +/- 0.00462\n",
      "       58/1    0.86482    0.85650 +/- 0.00452\n",
      "       59/1    0.85365    0.85644 +/- 0.00443\n",
      "       60/1    0.83314    0.85597 +/- 0.00437\n",
      "       61/1    0.87004    0.85625 +/- 0.00429\n",
      "       62/1    0.83331    0.85581 +/- 0.00423\n",
      "       63/1    0.81086    0.85496 +/- 0.00423\n",
      "       64/1    0.81488    0.85422 +/- 0.00422\n",
      "       65/1    0.78454    0.85295 +/- 0.00433\n",
      "       66/1    0.87513    0.85335 +/- 0.00427\n",
      "       67/1    0.87472    0.85372 +/- 0.00421\n",
      "       68/1    0.94228    0.85525 +/- 0.00441\n",
      "       69/1    0.85672    0.85527 +/- 0.00434\n",
      "       70/1    0.88222    0.85572 +/- 0.00429\n",
      "       71/1    0.92574    0.85687 +/- 0.00437\n",
      "       72/1    0.88145    0.85727 +/- 0.00432\n",
      "       73/1    0.88807    0.85776 +/- 0.00428\n",
      "       74/1    0.87056    0.85796 +/- 0.00421\n",
      "       75/1    0.85633    0.85793 +/- 0.00415\n",
      "       76/1    0.86664    0.85806 +/- 0.00409\n",
      "       77/1    0.84047    0.85780 +/- 0.00403\n",
      "       78/1    0.86840    0.85796 +/- 0.00398\n",
      "       79/1    0.85615    0.85793 +/- 0.00392\n",
      "       80/1    0.94059    0.85911 +/- 0.00404\n",
      "       81/1    0.88728    0.85951 +/- 0.00400\n",
      "       82/1    0.89945    0.86006 +/- 0.00398\n",
      "       83/1    0.84839    0.85990 +/- 0.00393\n",
      "       84/1    0.82529    0.85943 +/- 0.00391\n",
      "       85/1    0.77704    0.85834 +/- 0.00401\n",
      "       86/1    0.84615    0.85818 +/- 0.00396\n",
      "       87/1    0.82754    0.85778 +/- 0.00393\n",
      "       88/1    0.81986    0.85729 +/- 0.00391\n",
      "       89/1    0.81074    0.85670 +/- 0.00390\n",
      "       90/1    0.86281    0.85678 +/- 0.00385\n",
      "       91/1    0.83878    0.85656 +/- 0.00381\n",
      "       92/1    0.83633    0.85631 +/- 0.00377\n",
      "       93/1    0.87747    0.85656 +/- 0.00374\n",
      "       94/1    0.89484    0.85702 +/- 0.00372\n",
      "       95/1    0.81405    0.85651 +/- 0.00371\n",
      "       96/1    0.83776    0.85630 +/- 0.00367\n",
      "       97/1    0.82578    0.85595 +/- 0.00365\n",
      "       98/1    0.85177    0.85590 +/- 0.00361\n",
      "       99/1    0.83453    0.85566 +/- 0.00357\n",
      "      100/1    0.87937    0.85592 +/- 0.00354\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.2697e+00 seconds\n",
      "   Time in transport only          = 7.1053e+00 seconds\n",
      "   Time in inactive batches        = 2.6422e-01 seconds\n",
      "   Time in active batches          = 7.0055e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0514e-02 seconds\n",
      "     Sampling source sites         = 8.7512e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4475e-03 seconds\n",
      "   Time accumulating tallies       = 1.3464e-01 seconds\n",
      "   Time writing statepoints        = 6.6836e-03 seconds\n",
      " Total time for finalization       = 9.5990e-05 seconds\n",
      " Total time elapsed                = 7.2956e+00 seconds\n",
      " Calculation Rate (inactive)       = 37847.4 particles/second\n",
      " Calculation Rate (active)         = 12847.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.85655 +/- 0.00336\n",
      " k-effective (Track-length)  = 0.85592 +/- 0.00354\n",
      " k-effective (Absorption)    = 0.85151 +/- 0.00322\n",
      " Combined k-effective        = 0.85380 +/- 0.00265\n",
      " Leakage Fraction            = 0.13749 +/- 0.00126\n",
      "\n",
      " Creating state point openmc_simulation_n2.h5...\n",
      "[openmc.deplete] t=259200.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.54130\n",
      "        2/1    0.66035\n",
      "        3/1    0.76647\n",
      "        4/1    0.79829\n",
      "        5/1    0.76705\n",
      "        6/1    0.85986\n",
      "        7/1    0.88836\n",
      "        8/1    0.82032\n",
      "        9/1    0.83914\n",
      "       10/1    0.87351\n",
      "       11/1    0.86227\n",
      "       12/1    0.81926    0.84076 +/- 0.02150\n",
      "       13/1    0.89544    0.85899 +/- 0.02205\n",
      "       14/1    0.83257    0.85238 +/- 0.01693\n",
      "       15/1    0.85179    0.85226 +/- 0.01312\n",
      "       16/1    0.84263    0.85066 +/- 0.01083\n",
      "       17/1    0.84511    0.84987 +/- 0.00919\n",
      "       18/1    0.86623    0.85191 +/- 0.00821\n",
      "       19/1    0.89437    0.85663 +/- 0.00865\n",
      "       20/1    0.84886    0.85585 +/- 0.00777\n",
      "       21/1    0.84751    0.85509 +/- 0.00707\n",
      "       22/1    0.84215    0.85402 +/- 0.00654\n",
      "       23/1    0.77052    0.84759 +/- 0.00880\n",
      "       24/1    0.81061    0.84495 +/- 0.00857\n",
      "       25/1    0.85196    0.84542 +/- 0.00799\n",
      "       26/1    0.80174    0.84269 +/- 0.00796\n",
      "       27/1    0.81759    0.84121 +/- 0.00762\n",
      "       28/1    0.77620    0.83760 +/- 0.00804\n",
      "       29/1    0.76962    0.83402 +/- 0.00840\n",
      "       30/1    0.83751    0.83420 +/- 0.00797\n",
      "       31/1    0.87531    0.83616 +/- 0.00783\n",
      "       32/1    0.85077    0.83682 +/- 0.00750\n",
      "       33/1    0.85454    0.83759 +/- 0.00721\n",
      "       34/1    0.83081    0.83731 +/- 0.00691\n",
      "       35/1    0.75585    0.83405 +/- 0.00738\n",
      "       36/1    0.79627    0.83260 +/- 0.00724\n",
      "       37/1    0.85321    0.83336 +/- 0.00701\n",
      "       38/1    0.84271    0.83369 +/- 0.00676\n",
      "       39/1    0.89962    0.83597 +/- 0.00691\n",
      "       40/1    0.85102    0.83647 +/- 0.00669\n",
      "       41/1    0.82764    0.83618 +/- 0.00648\n",
      "       42/1    0.79437    0.83488 +/- 0.00641\n",
      "       43/1    0.82101    0.83446 +/- 0.00623\n",
      "       44/1    0.78847    0.83310 +/- 0.00619\n",
      "       45/1    0.80732    0.83237 +/- 0.00606\n",
      "       46/1    0.92040    0.83481 +/- 0.00637\n",
      "       47/1    0.94463    0.83778 +/- 0.00687\n",
      "       48/1    0.87188    0.83868 +/- 0.00675\n",
      "       49/1    0.77338    0.83700 +/- 0.00678\n",
      "       50/1    0.88589    0.83823 +/- 0.00672\n",
      "       51/1    0.88402    0.83934 +/- 0.00665\n",
      "       52/1    0.86889    0.84005 +/- 0.00653\n",
      "       53/1    0.82525    0.83970 +/- 0.00639\n",
      "       54/1    0.80894    0.83900 +/- 0.00628\n",
      "       55/1    0.90824    0.84054 +/- 0.00633\n",
      "       56/1    0.81618    0.84001 +/- 0.00621\n",
      "       57/1    0.87081    0.84067 +/- 0.00611\n",
      "       58/1    0.83088    0.84046 +/- 0.00599\n",
      "       59/1    0.82700    0.84019 +/- 0.00587\n",
      "       60/1    0.82539    0.83989 +/- 0.00576\n",
      "       61/1    0.76931    0.83851 +/- 0.00581\n",
      "       62/1    0.83740    0.83849 +/- 0.00570\n",
      "       63/1    0.88043    0.83928 +/- 0.00565\n",
      "       64/1    0.81456    0.83882 +/- 0.00556\n",
      "       65/1    0.87476    0.83947 +/- 0.00550\n",
      "       66/1    0.81062    0.83896 +/- 0.00542\n",
      "       67/1    0.83168    0.83883 +/- 0.00533\n",
      "       68/1    0.81481    0.83842 +/- 0.00525\n",
      "       69/1    0.81990    0.83810 +/- 0.00517\n",
      "       70/1    0.87470    0.83871 +/- 0.00512\n",
      "       71/1    0.88217    0.83943 +/- 0.00509\n",
      "       72/1    0.80549    0.83888 +/- 0.00503\n",
      "       73/1    0.86301    0.83926 +/- 0.00497\n",
      "       74/1    0.84245    0.83931 +/- 0.00489\n",
      "       75/1    0.84839    0.83945 +/- 0.00482\n",
      "       76/1    0.87148    0.83994 +/- 0.00477\n",
      "       77/1    0.89088    0.84070 +/- 0.00476\n",
      "       78/1    0.87206    0.84116 +/- 0.00471\n",
      "       79/1    0.89681    0.84196 +/- 0.00471\n",
      "       80/1    0.90906    0.84292 +/- 0.00474\n",
      "       81/1    0.84364    0.84293 +/- 0.00467\n",
      "       82/1    0.85661    0.84312 +/- 0.00461\n",
      "       83/1    0.87273    0.84353 +/- 0.00457\n",
      "       84/1    0.85307    0.84366 +/- 0.00450\n",
      "       85/1    0.82156    0.84336 +/- 0.00445\n",
      "       86/1    0.88670    0.84393 +/- 0.00443\n",
      "       87/1    0.87845    0.84438 +/- 0.00440\n",
      "       88/1    0.87640    0.84479 +/- 0.00436\n",
      "       89/1    0.87065    0.84512 +/- 0.00432\n",
      "       90/1    0.86786    0.84540 +/- 0.00427\n",
      "       91/1    0.82899    0.84520 +/- 0.00422\n",
      "       92/1    0.83230    0.84504 +/- 0.00417\n",
      "       93/1    0.83377    0.84491 +/- 0.00413\n",
      "       94/1    0.82312    0.84465 +/- 0.00409\n",
      "       95/1    0.82520    0.84442 +/- 0.00404\n",
      "       96/1    0.84067    0.84438 +/- 0.00400\n",
      "       97/1    0.80022    0.84387 +/- 0.00398\n",
      "       98/1    0.80180    0.84339 +/- 0.00397\n",
      "       99/1    0.83965    0.84335 +/- 0.00392\n",
      "      100/1    0.85139    0.84344 +/- 0.00388\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.4741e+00 seconds\n",
      "   Time in transport only          = 7.2669e+00 seconds\n",
      "   Time in inactive batches        = 2.6721e-01 seconds\n",
      "   Time in active batches          = 7.2069e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0686e-02 seconds\n",
      "     Sampling source sites         = 8.8384e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5517e-03 seconds\n",
      "   Time accumulating tallies       = 1.7900e-01 seconds\n",
      "   Time writing statepoints        = 6.5018e-03 seconds\n",
      " Total time for finalization       = 1.1451e-04 seconds\n",
      " Total time elapsed                = 7.5000e+00 seconds\n",
      " Calculation Rate (inactive)       = 37423.1 particles/second\n",
      " Calculation Rate (active)         = 12488.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84265 +/- 0.00372\n",
      " k-effective (Track-length)  = 0.84344 +/- 0.00388\n",
      " k-effective (Absorption)    = 0.84636 +/- 0.00350\n",
      " Combined k-effective        = 0.84478 +/- 0.00298\n",
      " Leakage Fraction            = 0.13916 +/- 0.00128\n",
      "\n",
      " Creating state point openmc_simulation_n3.h5...\n",
      "[openmc.deplete] t=345600.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50261\n",
      "        2/1    0.61659\n",
      "        3/1    0.72235\n",
      "        4/1    0.77766\n",
      "        5/1    0.91135\n",
      "        6/1    0.93872\n",
      "        7/1    0.84129\n",
      "        8/1    0.84685\n",
      "        9/1    0.80666\n",
      "       10/1    0.83596\n",
      "       11/1    0.83565\n",
      "       12/1    0.82372    0.82969 +/- 0.00596\n",
      "       13/1    0.83200    0.83046 +/- 0.00353\n",
      "       14/1    0.85312    0.83612 +/- 0.00619\n",
      "       15/1    0.85066    0.83903 +/- 0.00561\n",
      "       16/1    0.87342    0.84476 +/- 0.00734\n",
      "       17/1    0.85084    0.84563 +/- 0.00626\n",
      "       18/1    0.90004    0.85243 +/- 0.00870\n",
      "       19/1    0.88826    0.85641 +/- 0.00864\n",
      "       20/1    0.87981    0.85875 +/- 0.00808\n",
      "       21/1    0.79475    0.85293 +/- 0.00934\n",
      "       22/1    0.89647    0.85656 +/- 0.00927\n",
      "       23/1    0.92573    0.86188 +/- 0.01005\n",
      "       24/1    0.81436    0.85849 +/- 0.00990\n",
      "       25/1    0.88384    0.86018 +/- 0.00937\n",
      "       26/1    0.87421    0.86106 +/- 0.00881\n",
      "       27/1    0.83482    0.85951 +/- 0.00842\n",
      "       28/1    0.85641    0.85934 +/- 0.00794\n",
      "       29/1    0.84567    0.85862 +/- 0.00754\n",
      "       30/1    0.83054    0.85722 +/- 0.00729\n",
      "       31/1    0.77667    0.85338 +/- 0.00793\n",
      "       32/1    0.79095    0.85054 +/- 0.00807\n",
      "       33/1    0.85388    0.85069 +/- 0.00772\n",
      "       34/1    0.76830    0.84726 +/- 0.00815\n",
      "       35/1    0.90062    0.84939 +/- 0.00810\n",
      "       36/1    0.83854    0.84897 +/- 0.00779\n",
      "       37/1    0.79932    0.84713 +/- 0.00772\n",
      "       38/1    0.89427    0.84882 +/- 0.00763\n",
      "       39/1    0.86154    0.84926 +/- 0.00737\n",
      "       40/1    0.83169    0.84867 +/- 0.00715\n",
      "       41/1    0.89164    0.85006 +/- 0.00705\n",
      "       42/1    0.76101    0.84727 +/- 0.00737\n",
      "       43/1    0.85170    0.84741 +/- 0.00715\n",
      "       44/1    0.81197    0.84637 +/- 0.00701\n",
      "       45/1    0.86757    0.84697 +/- 0.00683\n",
      "       46/1    0.83530    0.84665 +/- 0.00665\n",
      "       47/1    0.81302    0.84574 +/- 0.00653\n",
      "       48/1    0.86183    0.84616 +/- 0.00637\n",
      "       49/1    0.85379    0.84636 +/- 0.00621\n",
      "       50/1    0.88525    0.84733 +/- 0.00613\n",
      "       51/1    0.83303    0.84698 +/- 0.00599\n",
      "       52/1    0.84287    0.84688 +/- 0.00584\n",
      "       53/1    0.87128    0.84745 +/- 0.00574\n",
      "       54/1    0.83449    0.84716 +/- 0.00561\n",
      "       55/1    0.85744    0.84738 +/- 0.00549\n",
      "       56/1    0.82461    0.84689 +/- 0.00539\n",
      "       57/1    0.77780    0.84542 +/- 0.00548\n",
      "       58/1    0.83466    0.84520 +/- 0.00537\n",
      "       59/1    0.78127    0.84389 +/- 0.00542\n",
      "       60/1    0.82930    0.84360 +/- 0.00531\n",
      "       61/1    0.89685    0.84464 +/- 0.00531\n",
      "       62/1    0.84507    0.84465 +/- 0.00521\n",
      "       63/1    0.87691    0.84526 +/- 0.00515\n",
      "       64/1    0.82472    0.84488 +/- 0.00506\n",
      "       65/1    0.82232    0.84447 +/- 0.00499\n",
      "       66/1    0.77823    0.84329 +/- 0.00504\n",
      "       67/1    0.81383    0.84277 +/- 0.00498\n",
      "       68/1    0.83421    0.84262 +/- 0.00489\n",
      "       69/1    0.82436    0.84231 +/- 0.00482\n",
      "       70/1    0.76926    0.84110 +/- 0.00489\n",
      "       71/1    0.84534    0.84116 +/- 0.00481\n",
      "       72/1    0.84237    0.84118 +/- 0.00473\n",
      "       73/1    0.83247    0.84105 +/- 0.00466\n",
      "       74/1    0.82591    0.84081 +/- 0.00459\n",
      "       75/1    0.83628    0.84074 +/- 0.00452\n",
      "       76/1    0.86479    0.84110 +/- 0.00447\n",
      "       77/1    0.83425    0.84100 +/- 0.00440\n",
      "       78/1    0.86166    0.84131 +/- 0.00435\n",
      "       79/1    0.91052    0.84231 +/- 0.00440\n",
      "       80/1    0.88278    0.84289 +/- 0.00437\n",
      "       81/1    0.87737    0.84337 +/- 0.00434\n",
      "       82/1    0.87931    0.84387 +/- 0.00431\n",
      "       83/1    0.86316    0.84414 +/- 0.00426\n",
      "       84/1    0.86378    0.84440 +/- 0.00421\n",
      "       85/1    0.81236    0.84397 +/- 0.00417\n",
      "       86/1    0.80173    0.84342 +/- 0.00415\n",
      "       87/1    0.81297    0.84302 +/- 0.00412\n",
      "       88/1    0.78318    0.84226 +/- 0.00414\n",
      "       89/1    0.84755    0.84232 +/- 0.00409\n",
      "       90/1    0.82448    0.84210 +/- 0.00404\n",
      "       91/1    0.85224    0.84223 +/- 0.00399\n",
      "       92/1    0.87695    0.84265 +/- 0.00397\n",
      "       93/1    0.81997    0.84238 +/- 0.00393\n",
      "       94/1    0.85612    0.84254 +/- 0.00388\n",
      "       95/1    0.90163    0.84323 +/- 0.00390\n",
      "       96/1    0.74285    0.84207 +/- 0.00403\n",
      "       97/1    0.84231    0.84207 +/- 0.00398\n",
      "       98/1    0.86028    0.84228 +/- 0.00394\n",
      "       99/1    0.82389    0.84207 +/- 0.00390\n",
      "      100/1    0.91500    0.84288 +/- 0.00394\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.0119e+00 seconds\n",
      "   Time in transport only          = 6.8624e+00 seconds\n",
      "   Time in inactive batches        = 2.6990e-01 seconds\n",
      "   Time in active batches          = 6.7420e+00 seconds\n",
      "   Time synchronizing fission bank = 1.4314e-02 seconds\n",
      "     Sampling source sites         = 1.2104e-02 seconds\n",
      "     SEND/RECV source sites        = 1.6934e-03 seconds\n",
      "   Time accumulating tallies       = 1.1426e-01 seconds\n",
      "   Time writing statepoints        = 6.7810e-03 seconds\n",
      " Total time for finalization       = 1.0625e-04 seconds\n",
      " Total time elapsed                = 7.0429e+00 seconds\n",
      " Calculation Rate (inactive)       = 37050.3 particles/second\n",
      " Calculation Rate (active)         = 13349.2 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84756 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.84288 +/- 0.00394\n",
      " k-effective (Absorption)    = 0.85177 +/- 0.00364\n",
      " Combined k-effective        = 0.84870 +/- 0.00300\n",
      " Leakage Fraction            = 0.13883 +/- 0.00114\n",
      "\n",
      " Creating state point openmc_simulation_n4.h5...\n",
      "[openmc.deplete] t=432000.0 (final operator evaluation)\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.52464\n",
      "        2/1    0.66396\n",
      "        3/1    0.75997\n",
      "        4/1    0.81762\n",
      "        5/1    0.79080\n",
      "        6/1    0.79719\n",
      "        7/1    0.84058\n",
      "        8/1    0.89457\n",
      "        9/1    0.87602\n",
      "       10/1    0.79190\n",
      "       11/1    0.89044\n",
      "       12/1    0.75483    0.82263 +/- 0.06780\n",
      "       13/1    0.83265    0.82597 +/- 0.03929\n",
      "       14/1    0.88418    0.84052 +/- 0.03136\n",
      "       15/1    0.86479    0.84538 +/- 0.02477\n",
      "       16/1    0.81151    0.83973 +/- 0.02100\n",
      "       17/1    0.82557    0.83771 +/- 0.01786\n",
      "       18/1    0.84485    0.83860 +/- 0.01550\n",
      "       19/1    0.81138    0.83558 +/- 0.01400\n",
      "       20/1    0.85383    0.83740 +/- 0.01265\n",
      "       21/1    0.86647    0.84005 +/- 0.01174\n",
      "       22/1    0.81713    0.83814 +/- 0.01089\n",
      "       23/1    0.85275    0.83926 +/- 0.01008\n",
      "       24/1    0.86851    0.84135 +/- 0.00956\n",
      "       25/1    0.84814    0.84180 +/- 0.00891\n",
      "       26/1    0.85268    0.84248 +/- 0.00837\n",
      "       27/1    0.91608    0.84681 +/- 0.00897\n",
      "       28/1    0.83835    0.84634 +/- 0.00847\n",
      "       29/1    0.81216    0.84454 +/- 0.00821\n",
      "       30/1    0.81024    0.84283 +/- 0.00798\n",
      "       31/1    0.79535    0.84057 +/- 0.00792\n",
      "       32/1    0.80667    0.83903 +/- 0.00771\n",
      "       33/1    0.84960    0.83948 +/- 0.00738\n",
      "       34/1    0.80292    0.83796 +/- 0.00723\n",
      "       35/1    0.82920    0.83761 +/- 0.00694\n",
      "       36/1    0.88990    0.83962 +/- 0.00696\n",
      "       37/1    0.82274    0.83900 +/- 0.00673\n",
      "       38/1    0.77730    0.83679 +/- 0.00685\n",
      "       39/1    0.85654    0.83747 +/- 0.00664\n",
      "       40/1    0.86892    0.83852 +/- 0.00650\n",
      "       41/1    0.90254    0.84059 +/- 0.00662\n",
      "       42/1    0.86666    0.84140 +/- 0.00646\n",
      "       43/1    0.86023    0.84197 +/- 0.00629\n",
      "       44/1    0.85197    0.84227 +/- 0.00611\n",
      "       45/1    0.79840    0.84101 +/- 0.00606\n",
      "       46/1    0.89092    0.84240 +/- 0.00605\n",
      "       47/1    0.91582    0.84438 +/- 0.00621\n",
      "       48/1    0.81594    0.84364 +/- 0.00609\n",
      "       49/1    0.81900    0.84300 +/- 0.00597\n",
      "       50/1    0.84671    0.84310 +/- 0.00582\n",
      "       51/1    0.88214    0.84405 +/- 0.00575\n",
      "       52/1    0.84352    0.84404 +/- 0.00561\n",
      "       53/1    0.86777    0.84459 +/- 0.00551\n",
      "       54/1    0.78129    0.84315 +/- 0.00557\n",
      "       55/1    0.85840    0.84349 +/- 0.00546\n",
      "       56/1    0.80863    0.84273 +/- 0.00539\n",
      "       57/1    0.82647    0.84238 +/- 0.00529\n",
      "       58/1    0.87793    0.84313 +/- 0.00523\n",
      "       59/1    0.81809    0.84261 +/- 0.00515\n",
      "       60/1    0.82066    0.84218 +/- 0.00506\n",
      "       61/1    0.82515    0.84184 +/- 0.00497\n",
      "       62/1    0.87484    0.84248 +/- 0.00492\n",
      "       63/1    0.87506    0.84309 +/- 0.00486\n",
      "       64/1    0.83154    0.84288 +/- 0.00478\n",
      "       65/1    0.76795    0.84151 +/- 0.00488\n",
      "       66/1    0.89135    0.84240 +/- 0.00488\n",
      "       67/1    0.82898    0.84217 +/- 0.00480\n",
      "       68/1    0.81531    0.84171 +/- 0.00473\n",
      "       69/1    0.83053    0.84152 +/- 0.00466\n",
      "       70/1    0.83328    0.84138 +/- 0.00458\n",
      "       71/1    0.78678    0.84048 +/- 0.00459\n",
      "       72/1    0.80836    0.83997 +/- 0.00455\n",
      "       73/1    0.80740    0.83945 +/- 0.00451\n",
      "       74/1    0.76353    0.83826 +/- 0.00459\n",
      "       75/1    0.88363    0.83896 +/- 0.00457\n",
      "       76/1    0.89715    0.83984 +/- 0.00459\n",
      "       77/1    0.88416    0.84050 +/- 0.00457\n",
      "       78/1    0.83159    0.84037 +/- 0.00450\n",
      "       79/1    0.89735    0.84120 +/- 0.00451\n",
      "       80/1    0.93387    0.84252 +/- 0.00464\n",
      "       81/1    0.82384    0.84226 +/- 0.00458\n",
      "       82/1    0.76773    0.84122 +/- 0.00464\n",
      "       83/1    0.86230    0.84151 +/- 0.00458\n",
      "       84/1    0.92572    0.84265 +/- 0.00466\n",
      "       85/1    0.79349    0.84200 +/- 0.00464\n",
      "       86/1    0.84166    0.84199 +/- 0.00458\n",
      "       87/1    0.79133    0.84133 +/- 0.00457\n",
      "       88/1    0.79088    0.84069 +/- 0.00456\n",
      "       89/1    0.85389    0.84085 +/- 0.00450\n",
      "       90/1    0.79765    0.84031 +/- 0.00448\n",
      "       91/1    0.82745    0.84015 +/- 0.00442\n",
      "       92/1    0.79995    0.83966 +/- 0.00440\n",
      "       93/1    0.82776    0.83952 +/- 0.00435\n",
      "       94/1    0.84485    0.83958 +/- 0.00430\n",
      "       95/1    0.90255    0.84032 +/- 0.00431\n",
      "       96/1    0.91112    0.84115 +/- 0.00434\n",
      "       97/1    0.82607    0.84097 +/- 0.00429\n",
      "       98/1    0.86315    0.84123 +/- 0.00425\n",
      "       99/1    0.85380    0.84137 +/- 0.00420\n",
      "      100/1    0.84776    0.84144 +/- 0.00416\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.3359e+00 seconds\n",
      "   Time in transport only          = 7.2143e+00 seconds\n",
      "   Time in inactive batches        = 2.4896e-01 seconds\n",
      "   Time in active batches          = 7.0870e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0501e-02 seconds\n",
      "     Sampling source sites         = 8.7494e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4779e-03 seconds\n",
      "   Time accumulating tallies       = 9.5154e-02 seconds\n",
      "   Time writing statepoints        = 6.5287e-03 seconds\n",
      " Total time for finalization       = 1.3627e-04 seconds\n",
      " Total time elapsed                = 7.3639e+00 seconds\n",
      " Calculation Rate (inactive)       = 40167.9 particles/second\n",
      " Calculation Rate (active)         = 12699.3 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84206 +/- 0.00355\n",
      " k-effective (Track-length)  = 0.84144 +/- 0.00416\n",
      " k-effective (Absorption)    = 0.83859 +/- 0.00275\n",
      " Combined k-effective        = 0.83961 +/- 0.00255\n",
      " Leakage Fraction            = 0.13700 +/- 0.00138\n",
      "\n",
      " Creating state point openmc_simulation_n5.h5...\n"
     ]
    }
   ],
   "source": [
    "chain_file = '/home/lorenzo/ca_depletion_chains/chain_simple.xml'\n",
    "uf4.volume = pi * fuel_or.r**2 * height\n",
    "op = openmc.deplete.CoupledOperator(model, chain_file)\n",
    "# Perform simulation using the predictor algorithm\n",
    "time_steps = [1.0, 1.0, 1.0, 1.0, 1.0]  # days\n",
    "power = 1.0e5  # W\n",
    "integrator = openmc.deplete.PredictorIntegrator(op, time_steps, power, timestep_units='d')\n",
    "integrator.integrate()"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "87ef9c7e",
   "metadata": {},
   "source": [
    "Let's store the results for later comparison"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 14,
   "id": "bcdcf2ff",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Open results file\n",
    "ref_results = openmc.deplete.Results(\"depletion_results.h5\")\n"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "db5a81b6",
   "metadata": {},
   "source": [
    "UF4 (assuming oxidation state of Uranium +4) frees 4 atoms of fluorine every time a fission event occurs, which will then bind with fission products with lower oxidation states than uranium, giving rise to an excess of free fluorine atoms and thus increasing the redox potential of the salt.  On the other hand, neutron capture reactions, will likely increase the oxidation state of the transmuting nuclide, thus creating a deficiency of fluorine atoms and reducing the redox potential of the salt.  \n",
    "Assuming the oxidation states of the nuclides present in the salt are known, the redox can be computed multiplying the number of atoms $N_i$ of each nuclide present in the salt, by their oxidation states $Ox_i$:\n",
    "\n",
    "\\begin{equation}\n",
    "\\sum_i N_i Ox_i\n",
    "\\end{equation}\n",
    "\n",
    "\n",
    "The added term for a generic buffer nuclide can be expressed mathematically  as: \n",
    "\n",
    "\\begin{equation}\n",
    "\\frac{dN_b(t)}{dt} = \\cdots + \\frac{1}{Ox_b}\\sum_i N_i\\left( L_{ii}Ox_i - \\sum_j G_{i\\rightarrow j } Ox_j\\right)\n",
    "\\end{equation}\n",
    "\n",
    "where `Ox_b` is the oxidation state of the buffer nuclide, and `Ox_i`, `Ox_j` are the oxidation states of the i-th nuclide undergoing a reaction or a decay and of the j-th product nuclide, respectively.\n",
    "Therefore, the first term in the right hand side represents the losses of the i-th nuclide (i.e. the diagonal terms of the Bateman matrix), and the second term the gains of the j-th nuclides (i.e. the off-diagonal terms of the Bateman matrix).\n",
    "\n",
    "To add a redox control to out fuel material, we have to add the `add_redox` method to an integrator instance, specifying the material to where add the routine, the nuclides buffer vector and a set of oxidation states. "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 15,
   "id": "561fee7d",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "                                %%%%%%%%%%%%%%%\n",
      "                           %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                        %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                      %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                    %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                    %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                     %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                 ###############      %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ##################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ###################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ####################     %%%%%%%%%%%%%%%%%%%%%%\n",
      "                #####################     %%%%%%%%%%%%%%%%%%%%%\n",
      "                ######################     %%%%%%%%%%%%%%%%%%%%\n",
      "                #######################     %%%%%%%%%%%%%%%%%%\n",
      "                 #######################     %%%%%%%%%%%%%%%%%\n",
      "                 ######################     %%%%%%%%%%%%%%%%%\n",
      "                  ####################     %%%%%%%%%%%%%%%%%\n",
      "                    #################     %%%%%%%%%%%%%%%%%\n",
      "                     ###############     %%%%%%%%%%%%%%%%\n",
      "                       ############     %%%%%%%%%%%%%%%\n",
      "                          ########     %%%%%%%%%%%%%%\n",
      "                                      %%%%%%%%%%%\n",
      "\n",
      "                 | The OpenMC Monte Carlo Code\n",
      "       Copyright | 2011-2024 MIT, UChicago Argonne LLC, and contributors\n",
      "         License | https://docs.openmc.org/en/latest/license.html\n",
      "         Version | 0.14.1-dev\n",
      "        Git SHA1 | d93ac83697e7fdb4fd4cc0f2705795398bf804bd\n",
      "       Date/Time | 2024-04-18 15:26:05\n",
      "   MPI Processes | 1\n",
      "  OpenMP Threads | 56\n",
      "\n",
      " Reading settings XML file...\n",
      " Reading cross sections XML file...\n",
      " Reading materials XML file...\n",
      " Reading geometry XML file...\n",
      " Reading U234 from /home/lorenzo/nuclear_data/endfb80_hdf5/U234.h5\n",
      " Reading U235 from /home/lorenzo/nuclear_data/endfb80_hdf5/U235.h5\n",
      " Reading U238 from /home/lorenzo/nuclear_data/endfb80_hdf5/U238.h5\n",
      " Reading F19 from /home/lorenzo/nuclear_data/endfb80_hdf5/F19.h5\n",
      " Reading U236 from /home/lorenzo/nuclear_data/endfb80_hdf5/U236.h5\n",
      " Reading He3 from /home/lorenzo/nuclear_data/endfb80_hdf5/He3.h5\n",
      " Reading He4 from /home/lorenzo/nuclear_data/endfb80_hdf5/He4.h5\n",
      " Reading Cr50 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr50.h5\n",
      " Reading Cr52 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr52.h5\n",
      " Reading Cr53 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr53.h5\n",
      " Reading Cr54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr54.h5\n",
      " Reading Fe54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe54.h5\n",
      " Reading Fe56 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe56.h5\n",
      " Reading Fe57 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe57.h5\n",
      " Reading Fe58 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe58.h5\n",
      " Reading Sn112 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn112.h5\n",
      " Reading Sn114 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn114.h5\n",
      " Reading Sn115 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn115.h5\n",
      " Reading Sn116 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn116.h5\n",
      " Reading Sn117 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn117.h5\n",
      " Reading Sn118 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn118.h5\n",
      " Reading Sn119 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn119.h5\n",
      " Reading Sn120 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn120.h5\n",
      " Reading Sn122 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn122.h5\n",
      " Reading Sn124 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn124.h5\n",
      " Reading Zr90 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr90.h5\n",
      " Reading Zr91 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr91.h5\n",
      " Reading Zr92 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr92.h5\n",
      " Reading Zr94 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr94.h5\n",
      " Reading Zr96 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr96.h5\n",
      " Reading B10 from /home/lorenzo/nuclear_data/endfb80_hdf5/B10.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Negative value(s) found on probability table for nuclide Zr96 at 294K\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading B11 from /home/lorenzo/nuclear_data/endfb80_hdf5/B11.h5\n",
      " Reading H1 from /home/lorenzo/nuclear_data/endfb80_hdf5/H1.h5\n",
      " Reading H2 from /home/lorenzo/nuclear_data/endfb80_hdf5/H2.h5\n",
      " Reading O16 from /home/lorenzo/nuclear_data/endfb80_hdf5/O16.h5\n",
      " Reading O17 from /home/lorenzo/nuclear_data/endfb80_hdf5/O17.h5\n",
      " Reading O18 from /home/lorenzo/nuclear_data/endfb80_hdf5/O18.h5\n",
      " Reading c_H_in_H2O from /home/lorenzo/nuclear_data/endfb80_hdf5/c_H_in_H2O.h5\n",
      " Minimum neutron data temperature: 0 K\n",
      " Maximum neutron data temperature: 1.7976931348623157e+308 K\n",
      " Reading tallies XML file...\n",
      " Preparing distributed cell instances...\n",
      " Reading plot XML file...\n",
      " Writing summary.h5 file...\n",
      "[openmc.deplete] t=0.0 s, dt=86400.0 s, source=100000.0\n",
      " Reading I135 from /home/lorenzo/nuclear_data/endfb80_hdf5/I135.h5\n",
      " Reading Xe135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe135.h5\n",
      " Reading Xe136 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe136.h5\n",
      " Reading Cs135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cs135.h5\n",
      " Reading Gd157 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd157.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Could not find material 5 specified in plot 1\n",
      " WARNING: Could not find material 6 specified in plot 1\n",
      " WARNING: Could not find material 7 specified in plot 1\n",
      " WARNING: Could not find material 8 specified in plot 1\n",
      " WARNING: Could not find material 9 specified in plot 1\n",
      " WARNING: Could not find material 10 specified in plot 1\n",
      " WARNING: Could not find material 5 specified in plot 2\n",
      " WARNING: Could not find material 6 specified in plot 2\n",
      " WARNING: Could not find material 7 specified in plot 2\n",
      " WARNING: Could not find material 8 specified in plot 2\n",
      " WARNING: Could not find material 9 specified in plot 2\n",
      " WARNING: Could not find material 10 specified in plot 2\n",
      " WARNING: Could not find material 5 specified in plot 3\n",
      " WARNING: Could not find material 6 specified in plot 3\n",
      " WARNING: Could not find material 7 specified in plot 3\n",
      " WARNING: Could not find material 8 specified in plot 3\n",
      " WARNING: Could not find material 9 specified in plot 3\n",
      " WARNING: Could not find material 10 specified in plot 3\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading Gd156 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd156.h5\n",
      " Reading Pu239 from /home/lorenzo/nuclear_data/endfb80_hdf5/Pu239.h5\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.55230\n",
      "        2/1    0.71581\n",
      "        3/1    0.84742\n",
      "        4/1    0.82083\n",
      "        5/1    0.88937\n",
      "        6/1    0.83661\n",
      "        7/1    0.90388\n",
      "        8/1    0.89892\n",
      "        9/1    0.84564\n",
      "       10/1    0.89387\n",
      "       11/1    0.81112\n",
      "       12/1    0.90903    0.86007 +/- 0.04896\n",
      "       13/1    0.82243    0.84752 +/- 0.03093\n",
      "       14/1    0.87888    0.85536 +/- 0.02323\n",
      "       15/1    0.85114    0.85452 +/- 0.01801\n",
      "       16/1    0.88721    0.85997 +/- 0.01569\n",
      "       17/1    0.88177    0.86308 +/- 0.01362\n",
      "       18/1    0.90888    0.86881 +/- 0.01311\n",
      "       19/1    0.83572    0.86513 +/- 0.01213\n",
      "       20/1    0.83936    0.86255 +/- 0.01115\n",
      "       21/1    0.94591    0.87013 +/- 0.01262\n",
      "       22/1    0.84293    0.86787 +/- 0.01174\n",
      "       23/1    0.88706    0.86934 +/- 0.01090\n",
      "       24/1    0.87462    0.86972 +/- 0.01010\n",
      "       25/1    0.77153    0.86317 +/- 0.01145\n",
      "       26/1    0.85637    0.86275 +/- 0.01072\n",
      "       27/1    0.80862    0.85956 +/- 0.01056\n",
      "       28/1    0.85113    0.85909 +/- 0.00997\n",
      "       29/1    0.83268    0.85770 +/- 0.00953\n",
      "       30/1    0.86520    0.85808 +/- 0.00905\n",
      "       31/1    0.93140    0.86157 +/- 0.00929\n",
      "       32/1    0.88934    0.86283 +/- 0.00895\n",
      "       33/1    0.87335    0.86329 +/- 0.00856\n",
      "       34/1    0.87573    0.86381 +/- 0.00821\n",
      "       35/1    0.91501    0.86586 +/- 0.00814\n",
      "       36/1    0.82385    0.86424 +/- 0.00799\n",
      "       37/1    0.82322    0.86272 +/- 0.00783\n",
      "       38/1    0.87062    0.86300 +/- 0.00755\n",
      "       39/1    0.86394    0.86304 +/- 0.00729\n",
      "       40/1    0.88725    0.86384 +/- 0.00709\n",
      "       41/1    0.88834    0.86463 +/- 0.00690\n",
      "       42/1    0.85313    0.86427 +/- 0.00669\n",
      "       43/1    0.93063    0.86629 +/- 0.00679\n",
      "       44/1    0.81729    0.86484 +/- 0.00674\n",
      "       45/1    0.79035    0.86272 +/- 0.00689\n",
      "       46/1    0.96206    0.86548 +/- 0.00724\n",
      "       47/1    0.88932    0.86612 +/- 0.00707\n",
      "       48/1    0.93670    0.86798 +/- 0.00713\n",
      "       49/1    0.88749    0.86848 +/- 0.00696\n",
      "       50/1    0.88210    0.86882 +/- 0.00679\n",
      "       51/1    0.83792    0.86806 +/- 0.00667\n",
      "       52/1    0.86035    0.86788 +/- 0.00651\n",
      "       53/1    0.83267    0.86706 +/- 0.00641\n",
      "       54/1    0.86629    0.86704 +/- 0.00626\n",
      "       55/1    0.83651    0.86637 +/- 0.00616\n",
      "       56/1    0.86899    0.86642 +/- 0.00602\n",
      "       57/1    0.86755    0.86645 +/- 0.00589\n",
      "       58/1    0.86296    0.86637 +/- 0.00577\n",
      "       59/1    0.90701    0.86720 +/- 0.00571\n",
      "       60/1    0.88598    0.86758 +/- 0.00561\n",
      "       61/1    0.83798    0.86700 +/- 0.00553\n",
      "       62/1    0.81695    0.86604 +/- 0.00551\n",
      "       63/1    0.90488    0.86677 +/- 0.00545\n",
      "       64/1    0.91599    0.86768 +/- 0.00543\n",
      "       65/1    0.85986    0.86754 +/- 0.00533\n",
      "       66/1    0.85999    0.86740 +/- 0.00523\n",
      "       67/1    0.88330    0.86768 +/- 0.00515\n",
      "       68/1    0.84368    0.86727 +/- 0.00508\n",
      "       69/1    0.86791    0.86728 +/- 0.00499\n",
      "       70/1    0.81372    0.86639 +/- 0.00499\n",
      "       71/1    0.87471    0.86652 +/- 0.00490\n",
      "       72/1    0.82349    0.86583 +/- 0.00487\n",
      "       73/1    0.92667    0.86679 +/- 0.00489\n",
      "       74/1    0.85169    0.86656 +/- 0.00482\n",
      "       75/1    0.83902    0.86614 +/- 0.00477\n",
      "       76/1    0.89600    0.86659 +/- 0.00471\n",
      "       77/1    0.86706    0.86659 +/- 0.00464\n",
      "       78/1    0.84111    0.86622 +/- 0.00459\n",
      "       79/1    0.80299    0.86530 +/- 0.00462\n",
      "       80/1    0.86359    0.86528 +/- 0.00455\n",
      "       81/1    0.80849    0.86448 +/- 0.00456\n",
      "       82/1    0.89804    0.86495 +/- 0.00452\n",
      "       83/1    0.86185    0.86490 +/- 0.00445\n",
      "       84/1    0.86501    0.86490 +/- 0.00439\n",
      "       85/1    0.84290    0.86461 +/- 0.00434\n",
      "       86/1    0.88679    0.86490 +/- 0.00430\n",
      "       87/1    0.92261    0.86565 +/- 0.00431\n",
      "       88/1    0.82757    0.86516 +/- 0.00428\n",
      "       89/1    0.87889    0.86534 +/- 0.00423\n",
      "       90/1    0.88855    0.86563 +/- 0.00418\n",
      "       91/1    0.85702    0.86552 +/- 0.00413\n",
      "       92/1    0.86806    0.86555 +/- 0.00408\n",
      "       93/1    0.88195    0.86575 +/- 0.00404\n",
      "       94/1    0.86865    0.86578 +/- 0.00399\n",
      "       95/1    0.89434    0.86612 +/- 0.00396\n",
      "       96/1    0.93531    0.86693 +/- 0.00399\n",
      "       97/1    0.91389    0.86747 +/- 0.00398\n",
      "       98/1    0.88900    0.86771 +/- 0.00395\n",
      "       99/1    0.86813    0.86771 +/- 0.00390\n",
      "      100/1    0.84827    0.86750 +/- 0.00386\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 3.2476e+00 seconds\n",
      "   Reading cross sections          = 3.2200e+00 seconds\n",
      " Total time in simulation          = 7.5407e+00 seconds\n",
      "   Time in transport only          = 7.3100e+00 seconds\n",
      "   Time in inactive batches        = 2.5203e-01 seconds\n",
      "   Time in active batches          = 7.2887e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1217e-02 seconds\n",
      "     Sampling source sites         = 9.3181e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5480e-03 seconds\n",
      "   Time accumulating tallies       = 2.0224e-01 seconds\n",
      "   Time writing statepoints        = 6.4992e-03 seconds\n",
      " Total time for finalization       = 1.1131e-04 seconds\n",
      " Total time elapsed                = 1.0812e+01 seconds\n",
      " Calculation Rate (inactive)       = 39677.1 particles/second\n",
      " Calculation Rate (active)         = 12347.9 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.87058 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.86750 +/- 0.00386\n",
      " k-effective (Absorption)    = 0.88032 +/- 0.00359\n",
      " Combined k-effective        = 0.87426 +/- 0.00317\n",
      " Leakage Fraction            = 0.13803 +/- 0.00134\n",
      "\n",
      " Creating state point openmc_simulation_n0.h5...\n",
      "[openmc.deplete] t=86400.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51707\n",
      "        2/1    0.67082\n",
      "        3/1    0.82109\n",
      "        4/1    0.84583\n",
      "        5/1    0.87260\n",
      "        6/1    0.82301\n",
      "        7/1    0.82349\n",
      "        8/1    0.87394\n",
      "        9/1    0.86266\n",
      "       10/1    0.78792\n",
      "       11/1    0.87132\n",
      "       12/1    0.83654    0.85393 +/- 0.01739\n",
      "       13/1    0.87749    0.86178 +/- 0.01275\n",
      "       14/1    0.85845    0.86095 +/- 0.00905\n",
      "       15/1    0.81697    0.85215 +/- 0.01125\n",
      "       16/1    0.88559    0.85773 +/- 0.01074\n",
      "       17/1    0.84292    0.85561 +/- 0.00932\n",
      "       18/1    0.89528    0.86057 +/- 0.00947\n",
      "       19/1    0.85057    0.85946 +/- 0.00843\n",
      "       20/1    0.91850    0.86536 +/- 0.00958\n",
      "       21/1    0.86457    0.86529 +/- 0.00866\n",
      "       22/1    0.84566    0.86366 +/- 0.00808\n",
      "       23/1    0.89270    0.86589 +/- 0.00776\n",
      "       24/1    0.87863    0.86680 +/- 0.00724\n",
      "       25/1    0.85908    0.86629 +/- 0.00676\n",
      "       26/1    0.79891    0.86207 +/- 0.00760\n",
      "       27/1    0.86269    0.86211 +/- 0.00714\n",
      "       28/1    0.89733    0.86407 +/- 0.00701\n",
      "       29/1    0.88634    0.86524 +/- 0.00673\n",
      "       30/1    0.86729    0.86534 +/- 0.00639\n",
      "       31/1    0.89035    0.86653 +/- 0.00619\n",
      "       32/1    0.93079    0.86945 +/- 0.00658\n",
      "       33/1    0.88108    0.86996 +/- 0.00631\n",
      "       34/1    0.91139    0.87169 +/- 0.00628\n",
      "       35/1    0.87858    0.87196 +/- 0.00603\n",
      "       36/1    0.81673    0.86984 +/- 0.00617\n",
      "       37/1    0.85152    0.86916 +/- 0.00598\n",
      "       38/1    0.82727    0.86766 +/- 0.00595\n",
      "       39/1    0.81996    0.86602 +/- 0.00598\n",
      "       40/1    0.81598    0.86435 +/- 0.00601\n",
      "       41/1    0.85644    0.86409 +/- 0.00582\n",
      "       42/1    0.96258    0.86717 +/- 0.00642\n",
      "       43/1    0.92079    0.86880 +/- 0.00643\n",
      "       44/1    0.86774    0.86877 +/- 0.00624\n",
      "       45/1    0.88135    0.86913 +/- 0.00607\n",
      "       46/1    0.81274    0.86756 +/- 0.00610\n",
      "       47/1    0.88937    0.86815 +/- 0.00596\n",
      "       48/1    0.86690    0.86812 +/- 0.00580\n",
      "       49/1    0.88990    0.86867 +/- 0.00568\n",
      "       50/1    0.88788    0.86915 +/- 0.00556\n",
      "       51/1    0.87508    0.86930 +/- 0.00542\n",
      "       52/1    0.81468    0.86800 +/- 0.00545\n",
      "       53/1    0.88567    0.86841 +/- 0.00534\n",
      "       54/1    0.82991    0.86753 +/- 0.00529\n",
      "       55/1    0.83443    0.86680 +/- 0.00522\n",
      "       56/1    0.91368    0.86782 +/- 0.00521\n",
      "       57/1    0.88560    0.86820 +/- 0.00511\n",
      "       58/1    0.85268    0.86787 +/- 0.00501\n",
      "       59/1    0.81537    0.86680 +/- 0.00502\n",
      "       60/1    0.84900    0.86645 +/- 0.00494\n",
      "       61/1    0.88650    0.86684 +/- 0.00485\n",
      "       62/1    0.90606    0.86759 +/- 0.00482\n",
      "       63/1    0.86394    0.86752 +/- 0.00473\n",
      "       64/1    0.90741    0.86826 +/- 0.00470\n",
      "       65/1    0.86143    0.86814 +/- 0.00461\n",
      "       66/1    0.85791    0.86796 +/- 0.00453\n",
      "       67/1    0.85604    0.86775 +/- 0.00446\n",
      "       68/1    0.89983    0.86830 +/- 0.00442\n",
      "       69/1    0.89514    0.86876 +/- 0.00436\n",
      "       70/1    0.90370    0.86934 +/- 0.00433\n",
      "       71/1    0.90941    0.86999 +/- 0.00431\n",
      "       72/1    0.86357    0.86989 +/- 0.00424\n",
      "       73/1    0.85397    0.86964 +/- 0.00418\n",
      "       74/1    0.86688    0.86960 +/- 0.00411\n",
      "       75/1    0.82833    0.86896 +/- 0.00410\n",
      "       76/1    0.85660    0.86877 +/- 0.00404\n",
      "       77/1    0.88298    0.86899 +/- 0.00399\n",
      "       78/1    0.86946    0.86899 +/- 0.00393\n",
      "       79/1    0.85507    0.86879 +/- 0.00387\n",
      "       80/1    0.89265    0.86913 +/- 0.00383\n",
      "       81/1    0.88248    0.86932 +/- 0.00378\n",
      "       82/1    0.87770    0.86944 +/- 0.00373\n",
      "       83/1    0.85861    0.86929 +/- 0.00368\n",
      "       84/1    0.85964    0.86916 +/- 0.00364\n",
      "       85/1    0.90793    0.86967 +/- 0.00363\n",
      "       86/1    0.87209    0.86971 +/- 0.00358\n",
      "       87/1    0.91591    0.87031 +/- 0.00358\n",
      "       88/1    0.85347    0.87009 +/- 0.00354\n",
      "       89/1    0.91173    0.87062 +/- 0.00354\n",
      "       90/1    0.78727    0.86957 +/- 0.00364\n",
      "       91/1    0.85006    0.86933 +/- 0.00361\n",
      "       92/1    0.86987    0.86934 +/- 0.00356\n",
      "       93/1    0.94632    0.87027 +/- 0.00364\n",
      "       94/1    0.89682    0.87058 +/- 0.00361\n",
      "       95/1    0.83969    0.87022 +/- 0.00359\n",
      "       96/1    0.88152    0.87035 +/- 0.00355\n",
      "       97/1    0.82912    0.86988 +/- 0.00354\n",
      "       98/1    0.89473    0.87016 +/- 0.00351\n",
      "       99/1    0.93193    0.87085 +/- 0.00354\n",
      "      100/1    0.95974    0.87184 +/- 0.00363\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.2523e+00 seconds\n",
      "   Time in transport only          = 7.0138e+00 seconds\n",
      "   Time in inactive batches        = 2.7262e-01 seconds\n",
      "   Time in active batches          = 6.9797e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1119e-02 seconds\n",
      "     Sampling source sites         = 9.2321e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4966e-03 seconds\n",
      "   Time accumulating tallies       = 2.0238e-01 seconds\n",
      "   Time writing statepoints        = 1.3119e-02 seconds\n",
      " Total time for finalization       = 1.1882e-04 seconds\n",
      " Total time elapsed                = 7.2816e+00 seconds\n",
      " Calculation Rate (inactive)       = 36681.4 particles/second\n",
      " Calculation Rate (active)         = 12894.6 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86782 +/- 0.00359\n",
      " k-effective (Track-length)  = 0.87184 +/- 0.00363\n",
      " k-effective (Absorption)    = 0.86805 +/- 0.00269\n",
      " Combined k-effective        = 0.86914 +/- 0.00241\n",
      " Leakage Fraction            = 0.13909 +/- 0.00131\n",
      "\n",
      " Creating state point openmc_simulation_n1.h5...\n",
      "[openmc.deplete] t=172800.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51231\n",
      "        2/1    0.62949\n",
      "        3/1    0.77894\n",
      "        4/1    0.77334\n",
      "        5/1    0.81725\n",
      "        6/1    0.81320\n",
      "        7/1    0.87094\n",
      "        8/1    0.88315\n",
      "        9/1    0.85332\n",
      "       10/1    0.88833\n",
      "       11/1    0.83211\n",
      "       12/1    0.85132    0.84171 +/- 0.00960\n",
      "       13/1    0.85203    0.84515 +/- 0.00652\n",
      "       14/1    0.84498    0.84511 +/- 0.00461\n",
      "       15/1    0.85259    0.84661 +/- 0.00387\n",
      "       16/1    0.87448    0.85125 +/- 0.00562\n",
      "       17/1    0.94973    0.86532 +/- 0.01485\n",
      "       18/1    0.85128    0.86356 +/- 0.01298\n",
      "       19/1    0.91120    0.86886 +/- 0.01261\n",
      "       20/1    0.89633    0.87161 +/- 0.01161\n",
      "       21/1    0.79878    0.86499 +/- 0.01241\n",
      "       22/1    0.83624    0.86259 +/- 0.01158\n",
      "       23/1    0.94509    0.86894 +/- 0.01240\n",
      "       24/1    0.86446    0.86862 +/- 0.01149\n",
      "       25/1    0.84100    0.86677 +/- 0.01085\n",
      "       26/1    0.81857    0.86376 +/- 0.01059\n",
      "       27/1    0.89350    0.86551 +/- 0.01010\n",
      "       28/1    0.93768    0.86952 +/- 0.01033\n",
      "       29/1    0.91051    0.87168 +/- 0.01001\n",
      "       30/1    0.89609    0.87290 +/- 0.00957\n",
      "       31/1    0.82167    0.87046 +/- 0.00942\n",
      "       32/1    0.86705    0.87030 +/- 0.00899\n",
      "       33/1    0.86055    0.86988 +/- 0.00860\n",
      "       34/1    0.83266    0.86833 +/- 0.00838\n",
      "       35/1    0.86830    0.86833 +/- 0.00804\n",
      "       36/1    0.82583    0.86669 +/- 0.00789\n",
      "       37/1    0.87269    0.86692 +/- 0.00760\n",
      "       38/1    0.88402    0.86753 +/- 0.00735\n",
      "       39/1    0.91334    0.86911 +/- 0.00726\n",
      "       40/1    0.84717    0.86838 +/- 0.00705\n",
      "       41/1    0.80127    0.86621 +/- 0.00716\n",
      "       42/1    0.87929    0.86662 +/- 0.00694\n",
      "       43/1    0.85853    0.86637 +/- 0.00673\n",
      "       44/1    0.83888    0.86557 +/- 0.00658\n",
      "       45/1    0.82229    0.86433 +/- 0.00651\n",
      "       46/1    0.88177    0.86481 +/- 0.00634\n",
      "       47/1    0.81652    0.86351 +/- 0.00631\n",
      "       48/1    0.83550    0.86277 +/- 0.00618\n",
      "       49/1    0.86065    0.86272 +/- 0.00602\n",
      "       50/1    0.89350    0.86349 +/- 0.00592\n",
      "       51/1    0.91940    0.86485 +/- 0.00593\n",
      "       52/1    0.87053    0.86499 +/- 0.00579\n",
      "       53/1    0.89560    0.86570 +/- 0.00570\n",
      "       54/1    0.92532    0.86705 +/- 0.00573\n",
      "       55/1    0.89254    0.86762 +/- 0.00563\n",
      "       56/1    0.85336    0.86731 +/- 0.00552\n",
      "       57/1    0.86488    0.86726 +/- 0.00540\n",
      "       58/1    0.88648    0.86766 +/- 0.00530\n",
      "       59/1    0.87044    0.86771 +/- 0.00519\n",
      "       60/1    0.88456    0.86805 +/- 0.00510\n",
      "       61/1    0.88523    0.86839 +/- 0.00501\n",
      "       62/1    0.92541    0.86948 +/- 0.00503\n",
      "       63/1    0.92812    0.87059 +/- 0.00506\n",
      "       64/1    0.89724    0.87108 +/- 0.00499\n",
      "       65/1    0.89409    0.87150 +/- 0.00491\n",
      "       66/1    0.80206    0.87026 +/- 0.00498\n",
      "       67/1    0.85710    0.87003 +/- 0.00490\n",
      "       68/1    0.84985    0.86968 +/- 0.00483\n",
      "       69/1    0.78165    0.86819 +/- 0.00497\n",
      "       70/1    0.84014    0.86772 +/- 0.00491\n",
      "       71/1    0.78608    0.86639 +/- 0.00501\n",
      "       72/1    0.89739    0.86689 +/- 0.00496\n",
      "       73/1    0.81139    0.86600 +/- 0.00496\n",
      "       74/1    0.87276    0.86611 +/- 0.00488\n",
      "       75/1    0.82314    0.86545 +/- 0.00485\n",
      "       76/1    0.84216    0.86510 +/- 0.00479\n",
      "       77/1    0.78307    0.86387 +/- 0.00487\n",
      "       78/1    0.88244    0.86415 +/- 0.00481\n",
      "       79/1    0.94495    0.86532 +/- 0.00488\n",
      "       80/1    0.84509    0.86503 +/- 0.00482\n",
      "       81/1    0.79560    0.86405 +/- 0.00485\n",
      "       82/1    0.92065    0.86484 +/- 0.00485\n",
      "       83/1    0.83230    0.86439 +/- 0.00480\n",
      "       84/1    0.92565    0.86522 +/- 0.00481\n",
      "       85/1    0.79162    0.86424 +/- 0.00484\n",
      "       86/1    0.88700    0.86454 +/- 0.00479\n",
      "       87/1    0.82213    0.86399 +/- 0.00476\n",
      "       88/1    0.80316    0.86321 +/- 0.00476\n",
      "       89/1    0.86255    0.86320 +/- 0.00470\n",
      "       90/1    0.91027    0.86379 +/- 0.00468\n",
      "       91/1    0.80112    0.86301 +/- 0.00468\n",
      "       92/1    0.85061    0.86286 +/- 0.00463\n",
      "       93/1    0.82748    0.86243 +/- 0.00459\n",
      "       94/1    0.93021    0.86324 +/- 0.00461\n",
      "       95/1    0.86288    0.86324 +/- 0.00455\n",
      "       96/1    0.82396    0.86278 +/- 0.00452\n",
      "       97/1    0.86367    0.86279 +/- 0.00447\n",
      "       98/1    0.81087    0.86220 +/- 0.00446\n",
      "       99/1    0.85040    0.86207 +/- 0.00441\n",
      "      100/1    0.86319    0.86208 +/- 0.00436\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.0348e+00 seconds\n",
      "   Time in transport only          = 6.7739e+00 seconds\n",
      "   Time in inactive batches        = 2.6225e-01 seconds\n",
      "   Time in active batches          = 6.7725e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1567e-02 seconds\n",
      "     Sampling source sites         = 9.6240e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5826e-03 seconds\n",
      "   Time accumulating tallies       = 2.3242e-01 seconds\n",
      "   Time writing statepoints        = 6.5365e-03 seconds\n",
      " Total time for finalization       = 1.3253e-04 seconds\n",
      " Total time elapsed                = 7.0621e+00 seconds\n",
      " Calculation Rate (inactive)       = 38131.8 particles/second\n",
      " Calculation Rate (active)         = 13289 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.85900 +/- 0.00399\n",
      " k-effective (Track-length)  = 0.86208 +/- 0.00436\n",
      " k-effective (Absorption)    = 0.86176 +/- 0.00419\n",
      " Combined k-effective        = 0.86136 +/- 0.00356\n",
      " Leakage Fraction            = 0.14041 +/- 0.00155\n",
      "\n",
      " Creating state point openmc_simulation_n2.h5...\n",
      "[openmc.deplete] t=259200.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.54126\n",
      "        2/1    0.74124\n",
      "        3/1    0.76683\n",
      "        4/1    0.79906\n",
      "        5/1    0.83065\n",
      "        6/1    0.91462\n",
      "        7/1    0.80641\n",
      "        8/1    0.84765\n",
      "        9/1    0.82454\n",
      "       10/1    0.86135\n",
      "       11/1    0.92166\n",
      "       12/1    0.89922    0.91044 +/- 0.01122\n",
      "       13/1    0.83750    0.88613 +/- 0.02516\n",
      "       14/1    0.89273    0.88778 +/- 0.01787\n",
      "       15/1    0.78147    0.86652 +/- 0.02537\n",
      "       16/1    0.81933    0.85865 +/- 0.02216\n",
      "       17/1    0.93603    0.86971 +/- 0.02174\n",
      "       18/1    0.84574    0.86671 +/- 0.01907\n",
      "       19/1    0.84101    0.86386 +/- 0.01706\n",
      "       20/1    0.88121    0.86559 +/- 0.01535\n",
      "       21/1    0.82215    0.86164 +/- 0.01444\n",
      "       22/1    0.89708    0.86459 +/- 0.01351\n",
      "       23/1    0.87759    0.86559 +/- 0.01247\n",
      "       24/1    0.87072    0.86596 +/- 0.01155\n",
      "       25/1    0.89621    0.86798 +/- 0.01094\n",
      "       26/1    0.84402    0.86648 +/- 0.01034\n",
      "       27/1    0.84700    0.86533 +/- 0.00978\n",
      "       28/1    0.83551    0.86368 +/- 0.00937\n",
      "       29/1    0.86485    0.86374 +/- 0.00886\n",
      "       30/1    0.85674    0.86339 +/- 0.00841\n",
      "       31/1    0.82877    0.86174 +/- 0.00817\n",
      "       32/1    0.87565    0.86237 +/- 0.00782\n",
      "       33/1    0.92857    0.86525 +/- 0.00800\n",
      "       34/1    0.95677    0.86906 +/- 0.00856\n",
      "       35/1    0.88529    0.86971 +/- 0.00824\n",
      "       36/1    0.90134    0.87093 +/- 0.00801\n",
      "       37/1    0.84064    0.86981 +/- 0.00778\n",
      "       38/1    0.79960    0.86730 +/- 0.00791\n",
      "       39/1    0.86605    0.86726 +/- 0.00763\n",
      "       40/1    0.94160    0.86974 +/- 0.00778\n",
      "       41/1    0.79668    0.86738 +/- 0.00788\n",
      "       42/1    0.89120    0.86812 +/- 0.00767\n",
      "       43/1    0.83896    0.86724 +/- 0.00749\n",
      "       44/1    0.86697    0.86723 +/- 0.00726\n",
      "       45/1    0.85518    0.86689 +/- 0.00706\n",
      "       46/1    0.86409    0.86681 +/- 0.00686\n",
      "       47/1    0.84118    0.86612 +/- 0.00671\n",
      "       48/1    0.85426    0.86581 +/- 0.00654\n",
      "       49/1    0.92953    0.86744 +/- 0.00657\n",
      "       50/1    0.86811    0.86746 +/- 0.00641\n",
      "       51/1    0.85972    0.86727 +/- 0.00625\n",
      "       52/1    0.86776    0.86728 +/- 0.00610\n",
      "       53/1    0.86252    0.86717 +/- 0.00596\n",
      "       54/1    0.91954    0.86836 +/- 0.00594\n",
      "       55/1    0.89106    0.86886 +/- 0.00583\n",
      "       56/1    0.77591    0.86684 +/- 0.00605\n",
      "       57/1    0.82251    0.86590 +/- 0.00600\n",
      "       58/1    0.89999    0.86661 +/- 0.00591\n",
      "       59/1    0.86183    0.86651 +/- 0.00579\n",
      "       60/1    0.81036    0.86539 +/- 0.00578\n",
      "       61/1    0.88939    0.86586 +/- 0.00569\n",
      "       62/1    0.93204    0.86713 +/- 0.00572\n",
      "       63/1    0.85342    0.86687 +/- 0.00562\n",
      "       64/1    0.82142    0.86603 +/- 0.00558\n",
      "       65/1    0.92041    0.86702 +/- 0.00556\n",
      "       66/1    0.88203    0.86729 +/- 0.00547\n",
      "       67/1    0.87129    0.86736 +/- 0.00537\n",
      "       68/1    0.90558    0.86802 +/- 0.00532\n",
      "       69/1    0.83280    0.86742 +/- 0.00526\n",
      "       70/1    0.85269    0.86718 +/- 0.00518\n",
      "       71/1    0.90796    0.86784 +/- 0.00514\n",
      "       72/1    0.76047    0.86611 +/- 0.00534\n",
      "       73/1    0.90983    0.86681 +/- 0.00530\n",
      "       74/1    0.88347    0.86707 +/- 0.00523\n",
      "       75/1    0.81100    0.86620 +/- 0.00522\n",
      "       76/1    0.85221    0.86599 +/- 0.00514\n",
      "       77/1    0.86402    0.86596 +/- 0.00507\n",
      "       78/1    0.85597    0.86582 +/- 0.00499\n",
      "       79/1    0.78746    0.86468 +/- 0.00505\n",
      "       80/1    0.94754    0.86586 +/- 0.00512\n",
      "       81/1    0.81149    0.86510 +/- 0.00510\n",
      "       82/1    0.92026    0.86586 +/- 0.00509\n",
      "       83/1    0.86860    0.86590 +/- 0.00502\n",
      "       84/1    0.89301    0.86627 +/- 0.00496\n",
      "       85/1    0.91839    0.86696 +/- 0.00494\n",
      "       86/1    0.86968    0.86700 +/- 0.00488\n",
      "       87/1    0.91921    0.86768 +/- 0.00486\n",
      "       88/1    0.82744    0.86716 +/- 0.00483\n",
      "       89/1    0.88698    0.86741 +/- 0.00477\n",
      "       90/1    0.89896    0.86781 +/- 0.00473\n",
      "       91/1    0.83428    0.86739 +/- 0.00469\n",
      "       92/1    0.88844    0.86765 +/- 0.00464\n",
      "       93/1    0.88211    0.86782 +/- 0.00459\n",
      "       94/1    0.79329    0.86694 +/- 0.00462\n",
      "       95/1    0.86330    0.86689 +/- 0.00456\n",
      "       96/1    0.84118    0.86659 +/- 0.00452\n",
      "       97/1    0.81229    0.86597 +/- 0.00451\n",
      "       98/1    0.88348    0.86617 +/- 0.00446\n",
      "       99/1    0.93234    0.86691 +/- 0.00447\n",
      "      100/1    0.77646    0.86591 +/- 0.00454\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.1013e+00 seconds\n",
      "   Time in transport only          = 6.9449e+00 seconds\n",
      "   Time in inactive batches        = 2.4343e-01 seconds\n",
      "   Time in active batches          = 6.8579e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0243e-02 seconds\n",
      "     Sampling source sites         = 8.4507e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4929e-03 seconds\n",
      "   Time accumulating tallies       = 1.2522e-01 seconds\n",
      "   Time writing statepoints        = 7.3460e-03 seconds\n",
      " Total time for finalization       = 1.1160e-04 seconds\n",
      " Total time elapsed                = 7.1259e+00 seconds\n",
      " Calculation Rate (inactive)       = 41079.7 particles/second\n",
      " Calculation Rate (active)         = 13123.6 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86664 +/- 0.00354\n",
      " k-effective (Track-length)  = 0.86591 +/- 0.00454\n",
      " k-effective (Absorption)    = 0.86870 +/- 0.00303\n",
      " Combined k-effective        = 0.86805 +/- 0.00282\n",
      " Leakage Fraction            = 0.13650 +/- 0.00123\n",
      "\n",
      " Creating state point openmc_simulation_n3.h5...\n",
      "[openmc.deplete] t=345600.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.49610\n",
      "        2/1    0.60587\n",
      "        3/1    0.77896\n",
      "        4/1    0.77892\n",
      "        5/1    0.91214\n",
      "        6/1    0.86581\n",
      "        7/1    0.87650\n",
      "        8/1    0.89453\n",
      "        9/1    0.88254\n",
      "       10/1    0.85943\n",
      "       11/1    0.92807\n",
      "       12/1    0.82771    0.87789 +/- 0.05018\n",
      "       13/1    0.89658    0.88412 +/- 0.02963\n",
      "       14/1    0.87571    0.88202 +/- 0.02106\n",
      "       15/1    0.90590    0.88680 +/- 0.01700\n",
      "       16/1    0.88850    0.88708 +/- 0.01388\n",
      "       17/1    0.82761    0.87858 +/- 0.01448\n",
      "       18/1    0.83552    0.87320 +/- 0.01365\n",
      "       19/1    0.87095    0.87295 +/- 0.01204\n",
      "       20/1    0.85805    0.87146 +/- 0.01087\n",
      "       21/1    0.88702    0.87287 +/- 0.00994\n",
      "       22/1    0.84382    0.87045 +/- 0.00939\n",
      "       23/1    0.84675    0.86863 +/- 0.00883\n",
      "       24/1    0.92756    0.87284 +/- 0.00919\n",
      "       25/1    0.92861    0.87656 +/- 0.00933\n",
      "       26/1    0.89704    0.87784 +/- 0.00882\n",
      "       27/1    0.84002    0.87561 +/- 0.00858\n",
      "       28/1    0.84253    0.87378 +/- 0.00829\n",
      "       29/1    0.85536    0.87281 +/- 0.00791\n",
      "       30/1    0.83396    0.87086 +/- 0.00775\n",
      "       31/1    0.89790    0.87215 +/- 0.00748\n",
      "       32/1    0.89601    0.87324 +/- 0.00721\n",
      "       33/1    0.91824    0.87519 +/- 0.00717\n",
      "       34/1    0.81655    0.87275 +/- 0.00728\n",
      "       35/1    0.81590    0.87047 +/- 0.00735\n",
      "       36/1    0.85682    0.86995 +/- 0.00708\n",
      "       37/1    0.87520    0.87014 +/- 0.00681\n",
      "       38/1    0.85936    0.86976 +/- 0.00658\n",
      "       39/1    0.83430    0.86854 +/- 0.00646\n",
      "       40/1    0.87716    0.86882 +/- 0.00625\n",
      "       41/1    0.84543    0.86807 +/- 0.00609\n",
      "       42/1    0.91044    0.86939 +/- 0.00605\n",
      "       43/1    0.88822    0.86996 +/- 0.00589\n",
      "       44/1    0.85919    0.86965 +/- 0.00572\n",
      "       45/1    0.93465    0.87150 +/- 0.00586\n",
      "       46/1    0.89929    0.87228 +/- 0.00574\n",
      "       47/1    0.84760    0.87161 +/- 0.00563\n",
      "       48/1    0.87833    0.87179 +/- 0.00548\n",
      "       49/1    0.86577    0.87163 +/- 0.00534\n",
      "       50/1    0.84803    0.87104 +/- 0.00524\n",
      "       51/1    0.86874    0.87099 +/- 0.00511\n",
      "       52/1    0.88816    0.87139 +/- 0.00500\n",
      "       53/1    0.85696    0.87106 +/- 0.00490\n",
      "       54/1    0.85910    0.87079 +/- 0.00479\n",
      "       55/1    0.83717    0.87004 +/- 0.00474\n",
      "       56/1    0.82645    0.86909 +/- 0.00473\n",
      "       57/1    0.84019    0.86848 +/- 0.00467\n",
      "       58/1    0.90658    0.86927 +/- 0.00464\n",
      "       59/1    0.91814    0.87027 +/- 0.00465\n",
      "       60/1    0.85346    0.86993 +/- 0.00457\n",
      "       61/1    0.86652    0.86987 +/- 0.00448\n",
      "       62/1    0.85954    0.86967 +/- 0.00440\n",
      "       63/1    0.86122    0.86951 +/- 0.00432\n",
      "       64/1    0.84353    0.86903 +/- 0.00427\n",
      "       65/1    0.80681    0.86790 +/- 0.00434\n",
      "       66/1    0.88680    0.86823 +/- 0.00427\n",
      "       67/1    0.78746    0.86682 +/- 0.00443\n",
      "       68/1    0.84505    0.86644 +/- 0.00437\n",
      "       69/1    0.90629    0.86712 +/- 0.00435\n",
      "       70/1    0.88362    0.86739 +/- 0.00428\n",
      "       71/1    0.87304    0.86748 +/- 0.00421\n",
      "       72/1    0.89332    0.86790 +/- 0.00417\n",
      "       73/1    0.84752    0.86758 +/- 0.00411\n",
      "       74/1    0.92472    0.86847 +/- 0.00414\n",
      "       75/1    0.82738    0.86784 +/- 0.00413\n",
      "       76/1    0.82643    0.86721 +/- 0.00411\n",
      "       77/1    0.93419    0.86821 +/- 0.00417\n",
      "       78/1    0.84689    0.86790 +/- 0.00412\n",
      "       79/1    0.86858    0.86791 +/- 0.00406\n",
      "       80/1    0.81155    0.86710 +/- 0.00409\n",
      "       81/1    0.86662    0.86709 +/- 0.00403\n",
      "       82/1    0.85116    0.86687 +/- 0.00398\n",
      "       83/1    0.87058    0.86692 +/- 0.00392\n",
      "       84/1    0.89582    0.86731 +/- 0.00389\n",
      "       85/1    0.92856    0.86813 +/- 0.00392\n",
      "       86/1    0.84282    0.86780 +/- 0.00388\n",
      "       87/1    0.94044    0.86874 +/- 0.00395\n",
      "       88/1    0.86037    0.86863 +/- 0.00390\n",
      "       89/1    0.81650    0.86797 +/- 0.00391\n",
      "       90/1    0.81930    0.86737 +/- 0.00390\n",
      "       91/1    0.85265    0.86718 +/- 0.00386\n",
      "       92/1    0.82454    0.86666 +/- 0.00385\n",
      "       93/1    0.88664    0.86690 +/- 0.00381\n",
      "       94/1    0.85404    0.86675 +/- 0.00377\n",
      "       95/1    0.87330    0.86683 +/- 0.00372\n",
      "       96/1    0.90474    0.86727 +/- 0.00371\n",
      "       97/1    0.89806    0.86762 +/- 0.00368\n",
      "       98/1    0.88225    0.86779 +/- 0.00364\n",
      "       99/1    0.89469    0.86809 +/- 0.00361\n",
      "      100/1    0.88764    0.86831 +/- 0.00358\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.1550e+00 seconds\n",
      "   Time in transport only          = 6.9803e+00 seconds\n",
      "   Time in inactive batches        = 2.7285e-01 seconds\n",
      "   Time in active batches          = 6.8821e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1270e-02 seconds\n",
      "     Sampling source sites         = 9.3598e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5631e-03 seconds\n",
      "   Time accumulating tallies       = 1.4263e-01 seconds\n",
      "   Time writing statepoints        = 7.9281e-03 seconds\n",
      " Total time for finalization       = 1.6731e-04 seconds\n",
      " Total time elapsed                = 7.1863e+00 seconds\n",
      " Calculation Rate (inactive)       = 36650.4 particles/second\n",
      " Calculation Rate (active)         = 13077.3 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86637 +/- 0.00351\n",
      " k-effective (Track-length)  = 0.86831 +/- 0.00358\n",
      " k-effective (Absorption)    = 0.86181 +/- 0.00317\n",
      " Combined k-effective        = 0.86450 +/- 0.00272\n",
      " Leakage Fraction            = 0.13627 +/- 0.00139\n",
      "\n",
      " Creating state point openmc_simulation_n4.h5...\n",
      "[openmc.deplete] t=432000.0 (final operator evaluation)\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51382\n",
      "        2/1    0.68087\n",
      "        3/1    0.81760\n",
      "        4/1    0.78992\n",
      "        5/1    0.94733\n",
      "        6/1    0.80371\n",
      "        7/1    0.88763\n",
      "        8/1    0.87331\n",
      "        9/1    0.81481\n",
      "       10/1    0.82082\n",
      "       11/1    0.89920\n",
      "       12/1    0.87289    0.88605 +/- 0.01316\n",
      "       13/1    0.83485    0.86898 +/- 0.01868\n",
      "       14/1    0.82625    0.85830 +/- 0.01699\n",
      "       15/1    0.87176    0.86099 +/- 0.01343\n",
      "       16/1    0.81098    0.85265 +/- 0.01378\n",
      "       17/1    0.85864    0.85351 +/- 0.01167\n",
      "       18/1    0.76667    0.84265 +/- 0.01483\n",
      "       19/1    0.86035    0.84462 +/- 0.01323\n",
      "       20/1    0.96359    0.85652 +/- 0.01678\n",
      "       21/1    0.87982    0.85864 +/- 0.01532\n",
      "       22/1    0.82207    0.85559 +/- 0.01432\n",
      "       23/1    0.84364    0.85467 +/- 0.01320\n",
      "       24/1    0.91063    0.85867 +/- 0.01286\n",
      "       25/1    0.88943    0.86072 +/- 0.01215\n",
      "       26/1    0.90590    0.86354 +/- 0.01171\n",
      "       27/1    0.81918    0.86093 +/- 0.01130\n",
      "       28/1    0.80515    0.85783 +/- 0.01110\n",
      "       29/1    0.85665    0.85777 +/- 0.01050\n",
      "       30/1    0.88173    0.85897 +/- 0.01003\n",
      "       31/1    0.87818    0.85988 +/- 0.00958\n",
      "       32/1    0.84638    0.85927 +/- 0.00916\n",
      "       33/1    0.87116    0.85979 +/- 0.00877\n",
      "       34/1    0.88029    0.86064 +/- 0.00844\n",
      "       35/1    0.89940    0.86219 +/- 0.00824\n",
      "       36/1    0.82353    0.86070 +/- 0.00806\n",
      "       37/1    0.82112    0.85924 +/- 0.00789\n",
      "       38/1    0.87667    0.85986 +/- 0.00763\n",
      "       39/1    0.87635    0.86043 +/- 0.00738\n",
      "       40/1    0.80497    0.85858 +/- 0.00737\n",
      "       41/1    0.88913    0.85957 +/- 0.00719\n",
      "       42/1    0.84952    0.85925 +/- 0.00697\n",
      "       43/1    0.90553    0.86065 +/- 0.00690\n",
      "       44/1    0.91362    0.86221 +/- 0.00687\n",
      "       45/1    0.86677    0.86234 +/- 0.00668\n",
      "       46/1    0.88106    0.86286 +/- 0.00651\n",
      "       47/1    0.92973    0.86467 +/- 0.00658\n",
      "       48/1    0.78168    0.86249 +/- 0.00677\n",
      "       49/1    0.91789    0.86391 +/- 0.00674\n",
      "       50/1    0.86431    0.86392 +/- 0.00657\n",
      "       51/1    0.83048    0.86310 +/- 0.00646\n",
      "       52/1    0.87701    0.86343 +/- 0.00632\n",
      "       53/1    0.82866    0.86262 +/- 0.00622\n",
      "       54/1    0.87095    0.86281 +/- 0.00608\n",
      "       55/1    0.85480    0.86263 +/- 0.00595\n",
      "       56/1    0.83655    0.86207 +/- 0.00584\n",
      "       57/1    0.87794    0.86241 +/- 0.00573\n",
      "       58/1    0.86917    0.86255 +/- 0.00561\n",
      "       59/1    0.83111    0.86190 +/- 0.00553\n",
      "       60/1    0.88951    0.86246 +/- 0.00545\n",
      "       61/1    0.86002    0.86241 +/- 0.00534\n",
      "       62/1    0.88420    0.86283 +/- 0.00525\n",
      "       63/1    0.88296    0.86321 +/- 0.00517\n",
      "       64/1    0.88730    0.86365 +/- 0.00509\n",
      "       65/1    0.83619    0.86315 +/- 0.00502\n",
      "       66/1    0.80202    0.86206 +/- 0.00505\n",
      "       67/1    0.83283    0.86155 +/- 0.00499\n",
      "       68/1    0.88596    0.86197 +/- 0.00492\n",
      "       69/1    0.86613    0.86204 +/- 0.00483\n",
      "       70/1    0.89472    0.86259 +/- 0.00478\n",
      "       71/1    0.80557    0.86165 +/- 0.00480\n",
      "       72/1    0.80165    0.86068 +/- 0.00482\n",
      "       73/1    0.88860    0.86113 +/- 0.00476\n",
      "       74/1    0.82942    0.86063 +/- 0.00471\n",
      "       75/1    0.78739    0.85950 +/- 0.00477\n",
      "       76/1    0.75627    0.85794 +/- 0.00495\n",
      "       77/1    0.87551    0.85820 +/- 0.00489\n",
      "       78/1    0.90775    0.85893 +/- 0.00487\n",
      "       79/1    0.89388    0.85944 +/- 0.00482\n",
      "       80/1    0.88164    0.85975 +/- 0.00477\n",
      "       81/1    0.85548    0.85969 +/- 0.00470\n",
      "       82/1    0.95063    0.86096 +/- 0.00480\n",
      "       83/1    0.85450    0.86087 +/- 0.00474\n",
      "       84/1    0.93592    0.86188 +/- 0.00478\n",
      "       85/1    0.82000    0.86132 +/- 0.00475\n",
      "       86/1    0.87641    0.86152 +/- 0.00469\n",
      "       87/1    0.87399    0.86169 +/- 0.00463\n",
      "       88/1    0.90851    0.86229 +/- 0.00461\n",
      "       89/1    0.85316    0.86217 +/- 0.00455\n",
      "       90/1    0.91676    0.86285 +/- 0.00455\n",
      "       91/1    0.86041    0.86282 +/- 0.00449\n",
      "       92/1    0.82105    0.86231 +/- 0.00447\n",
      "       93/1    0.81803    0.86178 +/- 0.00444\n",
      "       94/1    0.81371    0.86121 +/- 0.00443\n",
      "       95/1    0.83968    0.86095 +/- 0.00438\n",
      "       96/1    0.88228    0.86120 +/- 0.00434\n",
      "       97/1    0.87699    0.86138 +/- 0.00429\n",
      "       98/1    0.76437    0.86028 +/- 0.00438\n",
      "       99/1    0.83680    0.86002 +/- 0.00434\n",
      "      100/1    0.89919    0.86045 +/- 0.00432\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 7.4628e+00 seconds\n",
      "   Time in transport only          = 7.2377e+00 seconds\n",
      "   Time in inactive batches        = 2.8810e-01 seconds\n",
      "   Time in active batches          = 7.1747e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0928e-02 seconds\n",
      "     Sampling source sites         = 9.0621e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4761e-03 seconds\n",
      "   Time accumulating tallies       = 1.9582e-01 seconds\n",
      "   Time writing statepoints        = 7.5940e-03 seconds\n",
      " Total time for finalization       = 1.0478e-04 seconds\n",
      " Total time elapsed                = 7.4904e+00 seconds\n",
      " Calculation Rate (inactive)       = 34709.8 particles/second\n",
      " Calculation Rate (active)         = 12544.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.85810 +/- 0.00372\n",
      " k-effective (Track-length)  = 0.86045 +/- 0.00432\n",
      " k-effective (Absorption)    = 0.85389 +/- 0.00338\n",
      " Combined k-effective        = 0.85604 +/- 0.00304\n",
      " Leakage Fraction            = 0.13662 +/- 0.00116\n",
      "\n",
      " Creating state point openmc_simulation_n5.h5...\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "       52/1    0.99612    0.99609 +/- 0.00534\n",
      "       53/1    1.03349    0.99696 +/- 0.00529\n",
      "       54/1    1.00859    0.99723 +/- 0.00517\n",
      "       55/1    1.01775    0.99768 +/- 0.00508\n",
      "       56/1    0.92832    0.99617 +/- 0.00519\n",
      "       57/1    0.93116    0.99479 +/- 0.00526\n",
      "       58/1    1.02899    0.99550 +/- 0.00520\n",
      "       59/1    0.99388    0.99547 +/- 0.00509\n",
      "       60/1    1.03489    0.99626 +/- 0.00505\n",
      "       61/1    0.97515    0.99584 +/- 0.00497\n",
      "       62/1    0.98673    0.99567 +/- 0.00488\n",
      "       63/1    0.93810    0.99458 +/- 0.00491\n",
      "       64/1    1.03245    0.99528 +/- 0.00487\n",
      "       65/1    0.98606    0.99512 +/- 0.00478\n",
      "       66/1    1.00775    0.99534 +/- 0.00470\n",
      "       67/1    0.96381    0.99479 +/- 0.00465\n",
      "       68/1    1.13116    0.99714 +/- 0.00514\n",
      "       69/1    0.99263    0.99706 +/- 0.00505\n",
      "       70/1    1.06626    0.99822 +/- 0.00510\n",
      "       71/1    0.94620    0.99736 +/- 0.00508\n",
      "       72/1    0.97634    0.99703 +/- 0.00501\n",
      "       73/1    1.04282    0.99775 +/- 0.00499\n",
      "       74/1    1.00948    0.99794 +/- 0.00491\n",
      "       75/1    0.94155    0.99707 +/- 0.00491\n",
      "       76/1    0.92606    0.99599 +/- 0.00496\n",
      "       77/1    0.99907    0.99604 +/- 0.00488\n",
      "       78/1    0.97985    0.99580 +/- 0.00482\n",
      "       79/1    0.95040    0.99514 +/- 0.00479\n",
      "       80/1    1.00809    0.99533 +/- 0.00472\n",
      "       81/1    1.00376    0.99545 +/- 0.00466\n",
      "       82/1    1.02465    0.99585 +/- 0.00461\n",
      "       83/1    1.01509    0.99611 +/- 0.00456\n",
      "       84/1    0.98973    0.99603 +/- 0.00449\n",
      "       85/1    1.06671    0.99697 +/- 0.00453\n",
      "       86/1    1.00450    0.99707 +/- 0.00447\n",
      "       87/1    0.96330    0.99663 +/- 0.00444\n",
      "       88/1    0.99976    0.99667 +/- 0.00438\n",
      "       89/1    0.97792    0.99643 +/- 0.00433\n",
      "       90/1    0.98794    0.99633 +/- 0.00428\n",
      "       91/1    0.95557    0.99582 +/- 0.00426\n",
      "       92/1    1.03036    0.99625 +/- 0.00422\n",
      "       93/1    1.01406    0.99646 +/- 0.00418\n",
      "       94/1    1.00834    0.99660 +/- 0.00413\n",
      "       95/1    1.03954    0.99711 +/- 0.00411\n",
      "       96/1    0.95580    0.99663 +/- 0.00409\n",
      "       97/1    1.03583    0.99708 +/- 0.00407\n",
      "       98/1    0.99040    0.99700 +/- 0.00402\n",
      "       99/1    0.92266    0.99617 +/- 0.00407\n",
      "      100/1    1.04376    0.99670 +/- 0.00406\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 3.5591e+00 seconds\n",
      "   Time in transport only          = 3.1358e+00 seconds\n",
      "   Time in inactive batches        = 4.3515e-01 seconds\n",
      "   Time in active batches          = 3.1240e+00 seconds\n",
      "   Time synchronizing fission bank = 1.3492e-02 seconds\n",
      "     Sampling source sites         = 1.1438e-02 seconds\n",
      "     SEND/RECV source sites        = 1.5843e-03 seconds\n",
      "   Time accumulating tallies       = 3.8472e-01 seconds\n",
      "   Time writing statepoints        = 8.4672e-03 seconds\n",
      " Total time for finalization       = 1.8534e-04 seconds\n",
      " Total time elapsed                = 3.5935e+00 seconds\n",
      " Calculation Rate (inactive)       = 22980.7 particles/second\n",
      " Calculation Rate (active)         = 28809.6 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.99905 +/- 0.00377\n",
      " k-effective (Track-length)  = 0.99670 +/- 0.00406\n",
      " k-effective (Absorption)    = 0.99998 +/- 0.00390\n",
      " Combined k-effective        = 0.99893 +/- 0.00325\n",
      " Leakage Fraction            = 0.10724 +/- 0.00113\n",
      "\n",
      " Creating state point openmc_simulation_n5.h5...\n"
     ]
    }
   ],
   "source": [
    "# We need to re-instanciate the operator and the integrator \n",
    "op = openmc.deplete.CoupledOperator(model, chain_file)\n",
    "integrator = openmc.deplete.PredictorIntegrator(op, time_steps, power, timestep_units='d')\n",
    "\n",
    "# my guess of oxidation states \n",
    "ox = {\n",
    "    'H': +1, 'He': 0, 'Li': +1, 'Be': +2, 'B': +3,  'C': 0,   'N': +3, 'O': -2,\n",
    "    'F': -1, 'Ne': 0, 'Na': +1, 'Mg': +2, 'Al': +3, 'Si': +4, 'P': -3, 'S': -2,\n",
    "    'Cl':-1, 'Ar': 0, 'K':  +1, 'Ca': +2, 'Sc': +3, 'Ti': +4, 'V': +5, 'Cr':+3,\n",
    "    'Mn':+2, 'Fe':+3, 'Co': +2, 'Ni': +2, 'Cu': +2, 'Zn': +2, 'Ga':+3, 'Ge':+2,\n",
    "    'As':+3, 'Se':-2, 'Br': -1, 'Kr':  0, 'Rb': +1, 'Sr': +2, 'Y': +3, 'Zr':+4,\n",
    "    'Nb':+6, 'Mo':+4, 'Tc': +4, 'Ru': +2, 'Rh': +3, 'Pd': +2, 'Ag':+1, 'Cd':+2,\n",
    "    'In':+3, 'Sn':+2, 'Sb': +3, 'Te': +2, 'I':  -1, 'Xe':  0, 'Cs':+1, 'Ba':+2,\n",
    "    'La':+3, 'Ce':+3, 'Pr': +3, 'Nd': +3, 'Pm': +3, 'Sm': +3, 'Eu':+3, 'Gd':+3,\n",
    "    'Tb':+3, 'Dy':+3, 'Ho': +3, 'Er': +3, 'Tm': +3, 'Yb': +3, 'Lu':+3, 'Hf':+4,\n",
    "    'Ta':+5, 'W': +4, 'Re': +4, 'Os': +4, 'Ir': +3, 'Pt': +2, 'Au':+3, 'Hg':+1,\n",
    "    'Tl':+1, 'Pb':+2, 'Bi': +3, 'Po': +2, 'At': -1, 'Rn':  0, 'Fr':+1, 'Ra':+2,\n",
    "    'Ac':+2, 'Th':+4, 'Pa': +4, 'U':  +4, 'Np': +4, 'Pu': +3, 'Am':+3, 'Cm':+3,\n",
    "    'Bk':+3, 'Cf':+3, 'Es': +3, 'Fm': +3, 'Md': +3, 'No': +2, 'Lr':+3\n",
    "    }\n",
    "\n",
    "# Add transfer rates for main absorbers to maintain an almost constant burnup \n",
    "integrator.add_transfer_rate(uf4, ['Xe', 'Kr'], 0.1)\n",
    "# Use U238 as buffer for redox control\n",
    "integrator.add_redox(uf4, {'U238':1}, ox)\n",
    "integrator.integrate()"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "fe7f1c7f-3829-4f24-86d3-38ce53a27d33",
   "metadata": {},
   "source": [
    "We can now compute the redox in the two cases:"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 38,
   "id": "518e8f3b",
   "metadata": {
    "scrolled": true
   },
   "outputs": [
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "results = openmc.deplete.Results(\"depletion_results.h5\")\n",
    "\n",
    "ref_redox = np.zeros(len(results))\n",
    "redox = np.zeros(len(results))\n",
    "\n",
    "for nuc in results[0].index_nuc:\n",
    "    ox_nuc = ox[re.split(r'\\d+', nuc)[0]]\n",
    "    ref_redox += ox_nuc*ref_results.get_atoms('1',nuc)[1]\n",
    "    redox += ox_nuc*results.get_atoms('1',nuc)[1]\n",
    "\n",
    "plt.plot(ref_redox, label='ref')\n",
    "plt.plot(redox, label='redox control')\n",
    "plt.xlabel('Time [d]')\n",
    "plt.ylabel(r'$\\sum_iN_iOx_i$')\n",
    "plt.legend()\n",
    "plt.show() "
   ]
  },
  {
   "cell_type": "markdown",
   "id": "ba6c18fc-26fc-4de3-b916-8983e4cb0553",
   "metadata": {},
   "source": [
    "As we can notice, in the second case the initial redox is kept constant by addition of buffer nuclide U238 that compensate the increase of fluorine atoms in the fuel salt:"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 42,
   "id": "1b5fa2ef-7cc2-4653-aeb6-3bb0e41a765e",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "plt.plot(ref_results.get_atoms('1', 'U238')[1], label='ref')\n",
    "plt.plot(results.get_atoms('1', 'U238')[1], label='redox control')\n",
    "plt.xlabel('Time [d]')\n",
    "plt.ylabel('N. of U238 atoms in UF4')\n",
    "plt.legend()\n",
    "plt.show() "
   ]
  }
 ],
 "metadata": {
  "kernelspec": {
   "display_name": "Python 3 (ipykernel)",
   "language": "python",
   "name": "python3"
  },
  "language_info": {
   "codemirror_mode": {
    "name": "ipython",
    "version": 3
   },
   "file_extension": ".py",
   "mimetype": "text/x-python",
   "name": "python",
   "nbconvert_exporter": "python",
   "pygments_lexer": "ipython3",
   "version": "3.10.12"
  }
 },
 "nbformat": 4,
 "nbformat_minor": 5
}