ecp-benchmarks/smr/build-assembly-long.py
2022-06-08 11:23:49 -05:00

186 lines
6.3 KiB
Python

#!/usr/bin/env python3
import argparse
from math import pi, isclose
from pathlib import Path
import numpy as np
from tqdm import tqdm
import openmc
from smr.materials import materials, clone
from smr.surfaces import surfs, lattice_pitch, pin_pitch, bottom_fuel_stack, \
top_active_core, pellet_OR, active_fuel_length
from smr.pins import pin_universes, make_stack
# Define command-line options
parser = argparse.ArgumentParser()
parser.add_argument('--multipole', action='store_true',
help='Use multipole cross sections')
parser.add_argument('--no-multipole', dest='multipole', action='store_false',
help='Do not use multipole cross sections')
parser.add_argument('--clone', action='store_true',
help='Clone materials for each cell instance')
parser.add_argument('--no-clone', dest='clone', action='store_false',
help='Do not clone materials for each cell instance')
parser.add_argument('-a', '--axial', type=int, default=100,
help='Number of axial subdivisions in fuel')
parser.add_argument('-d', '--depleted', action='store_true',
help='Whether UO2 compositions should represent depleted fuel')
parser.add_argument('-o', '--output-dir', type=Path, default=None)
parser.set_defaults(clone=False, multipole=True)
args = parser.parse_args()
# Make directory for inputs
if args.output_dir is None:
if args.depleted:
directory = Path('assembly-long-depleted')
else:
directory = Path('assembly-long-fresh')
else:
directory = args.output_dir
directory.mkdir(exist_ok=True)
rings = [0.1*pin_pitch, 0.2*pin_pitch]
assembly_long_surfs = [
surfs['bottom FR'],
surfs['bot active core'],
surfs['top active core'],
surfs['top pin plenum'],
surfs['top FR'],
surfs['bot upper nozzle'],
surfs['top upper nozzle']
]
univs = pin_universes(rings, args.axial, args.depleted)
fuel_univ = make_stack(
'Fuel (3.1%) stack no grid',
surfaces=assembly_long_surfs,
universes=[
univs['water pin'],
univs['end plug'],
univs['Fuel pin (3.1%) no grid'],
univs['pin plenum'],
univs['end plug'],
univs['water pin']
]
)
# Define the NumPy array indices for assembly locations where there
# may be CR guide tubes, instrument tubes and burnable absorbers
nonfuel_y = np.array([2,2,2,3,3,5,5,5,5,5,8,8,8,8,8,11,11,11,11,11,13,13,14,14,14])
nonfuel_x = np.array([5,8,11,3,13,2,5,8,11,14,2,5,8,11,14,2,5,8,11,14,3,13,5,8,11])
universes = np.full((17,17), fuel_univ)
universes[nonfuel_y, nonfuel_x] = univs['GT empty']
# Instantiate the lattice
lattice = openmc.RectLattice(name='Pin lattice')
lattice.lower_left = (-17.*pin_pitch/2., -17.*pin_pitch/2.)
lattice.pitch = (pin_pitch, pin_pitch)
lattice.universes = universes
# Add lattice to bounding cell
root_universe = openmc.Universe(name='Root universe')
cell = openmc.Cell(name='Lattice cell')
cell.fill = lattice
z_bounds = +surfs['bottom FR'] & -surfs['top FR']
cell.region = surfs['lat grid box inner'] & z_bounds
root_universe.add_cell(cell)
# Apply reflective boundaries on sides and vacuum on bottom/top
surfs['bottom FR'].boundary_type = 'vacuum'
surfs['top FR'].boundary_type = 'vacuum'
for halfspace in surfs['lat grid box inner']:
halfspace.surface.boundary_type = 'reflective'
# Define geometry with a single assembly
geometry = openmc.Geometry(root_universe)
h = active_fuel_length / args.axial
fuel_mats = {}
# Count the number of instances for each cell and material
if args.clone:
geometry.determine_paths(instances_only=True)
for cell in tqdm(geometry.get_all_material_cells().values(),
desc='Differentiating materials / assigning volume'):
if cell.fill in materials:
# Determine if this material is fuel
is_fuel = 'UO2 Fuel' in cell.fill.name
# Fill cell with list of "differentiated" materials if requested
if args.clone:
cell.fill = [clone(cell.fill) for i in range(cell.num_instances)]
# Determine volume of each fuel material
if is_fuel:
upper_right = cell.region.bounding_box[1]
if isclose(upper_right[0], rings[0]):
ri, ro = 0.0, rings[0]
elif isclose(upper_right[0], rings[1]):
ri, ro = rings[0], rings[1]
else:
ri, ro = rings[1], pellet_OR
if args.clone:
for mat in cell.fill:
mat.volume = pi * (ro*ro - ri*ri) * h
else:
# In non-clone mode, we still need to create a copy of the
# material for each ring since they get different volumes
if ri not in fuel_mats:
cell.fill = cell.fill.clone()
cell.fill.volume = pi * (ro*ro - ri*ri) * h
fuel_mats[ri] = cell.fill
else:
cell.fill = fuel_mats[ri]
else:
if args.clone:
for mat in cell.fill:
mat.volume = 1.0
else:
cell.fill.volume = 1.0
#### Create OpenMC "materials.xml" file
print('Getting materials...')
all_materials = geometry.get_all_materials()
print('Creating materials collection...')
materials = openmc.Materials(all_materials.values())
print('Exporting materials to XML...')
materials.export_to_xml(str(directory / 'materials.xml'))
#### Create OpenMC "geometry.xml" file
geometry.export_to_xml(str(directory / 'geometry.xml'))
#### Create OpenMC "settings.xml" file
# Construct uniform initial source distribution over fissionable zones
lower_left = (-lattice_pitch/2, -lattice_pitch/2, bottom_fuel_stack)
upper_right = (lattice_pitch/2, lattice_pitch/2, top_active_core)
source = openmc.source.Source(space=openmc.stats.Box(lower_left, upper_right))
source.space.only_fissionable = True
settings = openmc.Settings()
settings.batches = 200
settings.inactive = 100
settings.particles = 10000
settings.output = {'tallies': False, 'summary': False}
settings.source = source
settings.sourcepoint = {'write': False}
settings.temperature = {
'default': 531.5,
'method': 'interpolation',
'range': (500.0, 1300.0)
}
if args.multipole:
settings.temperature['multipole'] = True
settings.temperature['tolerance'] = 1000
settings.export_to_xml(str(directory / 'settings.xml'))