OpenMC/tests/regression_tests/deplete_decay_only/test.py
Paul Romano ac941f79e0
Add RectangularPrism and HexagonalPrism composite surfaces (#2739)
Co-authored-by: Patrick Shriwise <pshriwise@gmail.com>
2023-11-01 09:13:40 -05:00

103 lines
3.5 KiB
Python

""" Transport-free depletion test suite """
from pathlib import Path
import shutil
import numpy as np
import pytest
import openmc
import openmc.deplete
from openmc.deplete import CoupledOperator, IndependentOperator, MicroXS
@pytest.fixture(scope="module")
def model():
fuel = openmc.Material(name="uo2")
fuel.add_element("U", 1, percent_type="ao", enrichment=4.25)
fuel.add_element("O", 2)
fuel.add_nuclide("Xe135_m1", 1)
fuel.add_nuclide("Cs135_m1", 1)
fuel.set_density("g/cc", 10.4)
clad = openmc.Material(name="clad")
clad.add_element("Zr", 1)
clad.set_density("g/cc", 6)
water = openmc.Material(name="water")
water.add_element("O", 1)
water.add_element("H", 2)
water.set_density("g/cc", 1.0)
water.add_s_alpha_beta("c_H_in_H2O")
radii = [0.42, 0.45]
fuel.volume = np.pi * radii[0] ** 2
materials = openmc.Materials([fuel, clad, water])
pin_surfaces = [openmc.ZCylinder(r=r) for r in radii]
pin_univ = openmc.model.pin(pin_surfaces, materials)
bound_box = openmc.model.RectangularPrism(1.24, 1.24, boundary_type="reflective")
root_cell = openmc.Cell(fill=pin_univ, region=-bound_box)
geometry = openmc.Geometry([root_cell])
settings = openmc.Settings()
settings.particles = 1000
settings.inactive = 5
settings.batches = 10
return openmc.Model(geometry, materials, settings)
@pytest.fixture(scope="module")
def micro_xs():
micro_xs_file = Path(__file__).parents[2] / 'micro_xs_simple.csv'
return MicroXS.from_csv(micro_xs_file)
@pytest.fixture(scope="module")
def chain_file():
return Path(__file__).parents[2] / 'chain_simple_decay.xml'
@pytest.mark.parametrize("operator_type", ["coupled", "independent"])
def test_decay_only(run_in_tmpdir, operator_type, model, micro_xs, chain_file):
"""Transport free system test suite.
"""
# Create operator
if operator_type == "coupled":
op = CoupledOperator(model, chain_file=chain_file)
else:
op = IndependentOperator(openmc.Materials([model.materials[0]]),
[1e15],
[micro_xs],
chain_file)
# Power and timesteps
dt = [917.4, 2262.6] # one Xe135_m1 half life and one Cs135_m1 half life
# Perform simulation using the predictor algorithm
openmc.deplete.PredictorIntegrator(op,
dt,
power=0.0,
timestep_units='s').integrate()
# Get path to test and reference results
path_test = op.output_dir / 'depletion_results.h5'
# Load the reference/test results
res_test = openmc.deplete.Results(path_test)
_, xe135m1_atoms = res_test.get_atoms('1', 'Xe135_m1')
_, xe135_atoms = res_test.get_atoms('1', 'Xe135')
_, cs135m1_atoms = res_test.get_atoms('1', 'Cs135_m1')
_, cs135_atoms = res_test.get_atoms('1', 'Cs135')
tol = 1.0e-14
assert xe135m1_atoms[0] == pytest.approx(xe135m1_atoms[1] * 2, rel=tol)
# WARNING: this is generally not true as Xe135_m1 has two
# decay modes, and Xe135 will also decay, but we've modified the depletion chain so
# that Xe135_m1 only decays to Xe135, and that Xe135 has has no decay modes
assert xe135_atoms[1] == pytest.approx(xe135m1_atoms[1], rel=tol)
assert cs135m1_atoms[0] == pytest.approx(cs135m1_atoms[2] * 2, rel=tol)
assert cs135_atoms[2] == pytest.approx(cs135m1_atoms[2], rel=tol)