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https://github.com/openmc-dev/openmc.git
synced 2026-07-28 14:15:42 -04:00
Added test of convert_* methods;
This commit is contained in:
parent
130db90c2a
commit
384a08956a
4 changed files with 303 additions and 54 deletions
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@ -14,11 +14,14 @@ from openmc.checkvalue import check_type, check_value, check_greater_than, \
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# Supported incoming particle MGXS angular treatment representations
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_REPRESENTATIONS = ['isotropic', 'angle']
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# Supported scattering angular distribution representations
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_SCATTER_TYPES = ['tabular', 'legendre', 'histogram']
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# List of MGXS dimension types
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# List of MGXS indexing schemes
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_XS_SHAPES = ["[G][G'][Order]", "[G]", "[G']", "[G][G']", "[DG]", "[DG][G]",
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"[DG][G']", "[DG][G][G']"]
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# Number of mu points for conversion between scattering formats
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_NMU = 257
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@ -368,15 +371,14 @@ class XSdata(object):
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@name.setter
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def name(self, name):
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check_type('name for XSdata', name, string_types)
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self._name = name
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@energy_groups.setter
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def energy_groups(self, energy_groups):
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# Check validity of energy_groups
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check_type('energy_groups', energy_groups, openmc.mgxs.EnergyGroups)
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if energy_groups.group_edges is None:
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msg = 'Unable to assign an EnergyGroups object ' \
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'with uninitialized group edges'
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@ -387,7 +389,6 @@ class XSdata(object):
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@num_delayed_groups.setter
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def num_delayed_groups(self, num_delayed_groups):
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# Check validity of num_delayed_groups
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check_type('num_delayed_groups', num_delayed_groups, Integral)
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check_less_than('num_delayed_groups', num_delayed_groups,
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openmc.mgxs.MAX_DELAYED_GROUPS, equality=True)
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@ -398,14 +399,12 @@ class XSdata(object):
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@representation.setter
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def representation(self, representation):
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# Check it is of valid value.
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check_value('representation', representation, _REPRESENTATIONS)
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self._representation = representation
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@atomic_weight_ratio.setter
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def atomic_weight_ratio(self, atomic_weight_ratio):
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# Check validity of type and that the atomic_weight_ratio value is > 0
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check_type('atomic_weight_ratio', atomic_weight_ratio, Real)
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check_greater_than('atomic_weight_ratio', atomic_weight_ratio, 0.0)
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self._atomic_weight_ratio = atomic_weight_ratio
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@ -419,14 +418,12 @@ class XSdata(object):
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@scatter_format.setter
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def scatter_format(self, scatter_format):
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# check to see it is of a valid type and value
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check_value('scatter_format', scatter_format, _SCATTER_TYPES)
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self._scatter_format = scatter_format
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@order.setter
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def order(self, order):
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# Check type and value
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check_type('order', order, Integral)
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check_greater_than('order', order, 0, equality=True)
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self._order = order
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@ -434,7 +431,6 @@ class XSdata(object):
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@num_polar.setter
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def num_polar(self, num_polar):
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# Make sure we have positive ints
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check_type('num_polar', num_polar, Integral)
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check_greater_than('num_polar', num_polar, 0)
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self._num_polar = num_polar
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@ -1688,7 +1684,14 @@ class XSdata(object):
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def convert_representation(self, target_representation, num_polar=None,
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num_azimuthal=None):
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"""Produce a new XSdata object with the same data, but converted to the
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new representation
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new representation (isotropic or angle-dependent).
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This method cannot be used to change the number of polar or
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azimuthal bins of an XSdata object that already uses an angular
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representation. Finally, this method simply uses an arithmetic mean to
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convert from an angular to isotropic representation; no flux-weighting
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is applied and therefore the correctness of the solution is not
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guaranteed.
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Parameters
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----------
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@ -1728,9 +1731,9 @@ class XSdata(object):
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# Check to make sure the num_polar and num_azimuthal values match
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if target_representation == 'angle':
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if num_polar != self.num_polar or num_azimuthal != self.num_azimuthal:
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raise NotImplementedError("XCannot translate between "
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"`angle` representations with "
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"different angle bin structures")
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raise ValueError("Cannot translate between `angle`"
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" representations with different angle"
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" bin structures")
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# Nothing to do as the same structure was requested
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return xsdata
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@ -1741,6 +1744,7 @@ class XSdata(object):
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# values are changed back to None for clarity
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xsdata._num_polar = None
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xsdata._num_azimuthal = None
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elif target_representation == 'angle':
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xsdata.num_polar = num_polar
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xsdata.num_azimuthal = num_azimuthal
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@ -1757,16 +1761,19 @@ class XSdata(object):
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# Get the original data
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orig_data = getattr(self, '_' + xs)[i]
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if orig_data is not None:
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if target_representation == 'isotropic':
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# Since we are going from angle to isotropic, the
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# current data is just the average over the angle bins
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new_data = orig_data.mean(axis=(0, 1))
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elif target_representation == 'angle':
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# Since we are going from isotropic to angle, the
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# current data is just copied for every angle bin
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new_shape = (num_polar, num_azimuthal) + \
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orig_data.shape
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new_data = np.resize(orig_data, new_shape)
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setter = getattr(xsdata, 'set_' + xs)
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setter(new_data, temp)
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@ -1810,18 +1817,19 @@ class XSdata(object):
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# Reset and re-generate XSdata.xs_shapes with the new scattering format
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xsdata._xs_shapes = None
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xsdata.xs_shapes
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for i, temp in enumerate(xsdata.temperatures):
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orig_data = self._scatter_matrix[i]
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new_shape = orig_data.shape[:-1] + (xsdata.num_orders,)
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new_data = np.zeros(new_shape)
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if self.scatter_format == 'legendre':
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if target_format == 'legendre':
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# Then we are changing orders and only need to change
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# dimensionality of the mu data and pad/truncate as needed
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order = min(xsdata.num_orders, self.num_orders)
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new_data[..., :order] = orig_data[..., :order]
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elif target_format == 'tabular':
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mu = np.linspace(-1, 1, xsdata.num_orders)
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# Evaluate the legendre on the mu grid
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@ -1856,6 +1864,7 @@ class XSdata(object):
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elif self.scatter_format == 'tabular':
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# Calculate the mu points of the current data
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mu_self = np.linspace(-1, 1, self.num_orders)
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if target_format == 'legendre':
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# Find the Legendre coefficients via integration. To best
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# use the vectorized integration capabilities of scipy,
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@ -1870,10 +1879,12 @@ class XSdata(object):
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# Remove the very small values resulting from numerical
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# precision issues
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new_data[..., np.abs(new_data) < 1.E-10] = 0.
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elif target_format == 'tabular':
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# Simply use an interpolating function to get the new data
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mu = np.linspace(-1, 1, xsdata.num_orders)
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new_data[..., :] = interp1d(mu_self, orig_data)(mu)
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elif target_format == 'histogram':
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# Use an interpolating function to do the bin-wise
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# integrals
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@ -1891,6 +1902,7 @@ class XSdata(object):
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# Remove the very small values resulting from numerical
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# precision issues
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new_data[..., np.abs(new_data) < 1.E-10] = 0.
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elif self.scatter_format == 'histogram':
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# The histogram format does not have enough information to
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# convert to the other forms without inducing some amount of
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@ -1921,10 +1933,12 @@ class XSdata(object):
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# Remove the very small values resulting from numerical
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# precision issues
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new_data[..., np.abs(new_data) < 1.E-10] = 0.
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elif target_format == 'tabular':
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# Simply use an interpolating function to get the new data
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mu = np.linspace(-1, 1, xsdata.num_orders)
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new_data[..., :] = interp(mu) * norm
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elif target_format == 'histogram':
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# Use an interpolating function to do the bin-wise
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# integrals
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@ -1942,6 +1956,7 @@ class XSdata(object):
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# Remove the very small values resulting from numerical
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# precision issues
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new_data[..., np.abs(new_data) < 1.E-10] = 0.
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xsdata.set_scatter_matrix(new_data, temp)
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return xsdata
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@ -2431,8 +2446,15 @@ class MGXSLibrary(object):
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def convert_representation(self, target_representation, num_polar=None,
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num_azimuthal=None):
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"""Produce a new MGXSLibrary object with the same data, but converted
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to the new representation
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"""Produce a new XSdata object with the same data, but converted to the
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new representation (isotropic or angle-dependent).
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This method cannot be used to change the number of polar or
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azimuthal bins of an XSdata object that already uses an angular
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representation. Finally, this method simply uses an arithmetic mean to
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convert from an angular to isotropic representation; no flux-weighting
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is applied and therefore the correctness of the solution is not
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guaranteed.
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Parameters
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----------
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@ -2456,14 +2478,6 @@ class MGXSLibrary(object):
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"""
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check_value('target_representation', target_representation,
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_REPRESENTATIONS)
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if target_representation == 'angle':
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check_type('num_polar', num_polar, Integral)
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check_type('num_azimuthal', num_azimuthal, Integral)
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check_greater_than('num_polar', num_polar, 0)
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check_greater_than('num_azimuthal', num_azimuthal, 0)
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library = copy.deepcopy(self)
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for i, xsdata in enumerate(self.xsdatas):
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library.xsdatas[i] = \
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@ -2493,13 +2507,6 @@ class MGXSLibrary(object):
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"""
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check_value('target_format', target_format, _SCATTER_TYPES)
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check_type('target_order', target_order, Integral)
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if target_format == 'legendre':
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check_greater_than('target_order', target_order, 0, equality=True)
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else:
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check_greater_than('target_order', target_order, 0)
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library = copy.deepcopy(self)
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for i, xsdata in enumerate(self.xsdatas):
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library.xsdatas[i] = \
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@ -2507,29 +2514,6 @@ class MGXSLibrary(object):
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return library
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def convert_to_continuous_energy(self, h5_filename='ce_mgxs.h5',
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library_filename='ce_mgxs.xml'):
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"""Converts the MGXSLibrary object to an equivalent
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library of openmc.data.IncidentNeutron objects
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Parameters
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----------
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h5_filename : str
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HDF5 file to write with all the files
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library_filename : str
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cross_sections.xml file describing the HDF5 file
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"""
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library = openmc.data.DataLibrary()
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data = []
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for i, xsdata in enumerate(self.xsdatas):
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data.append(xsdata.convert_to_continuous_energy())
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data[-1].export_to_hdf5(h5_filename)
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library.register_file(h5_filename)
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library.export_to_xml(library_filename)
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def export_to_hdf5(self, filename='mgxs.h5'):
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"""Create an hdf5 file that can be used for a simulation.
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30
tests/test_mg_convert/inputs_true.dat
Normal file
30
tests/test_mg_convert/inputs_true.dat
Normal file
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@ -0,0 +1,30 @@
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<?xml version='1.0' encoding='utf-8'?>
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<geometry>
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<cell id="1" material="1" name="cell 1" region="4 -5 6 -7" universe="0" />
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<surface boundary="reflective" coeffs="-5.0" id="4" name="left" type="x-plane" />
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<surface boundary="vacuum" coeffs="5.0" id="5" name="right" type="x-plane" />
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<surface boundary="reflective" coeffs="-5.0" id="6" name="bottom" type="y-plane" />
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<surface boundary="reflective" coeffs="5.0" id="7" name="top" type="y-plane" />
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</geometry>
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<?xml version='1.0' encoding='utf-8'?>
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<materials>
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<cross_sections>./mgxs.h5</cross_sections>
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<material id="1" name="UO2 fuel">
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<density units="macro" value="1.0" />
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<macroscopic name="UO2" />
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</material>
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</materials>
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<?xml version='1.0' encoding='utf-8'?>
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<settings>
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<eigenvalue>
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<particles>1000</particles>
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<batches>2000</batches>
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<inactive>100</inactive>
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</eigenvalue>
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<source strength="1.0">
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<space type="box">
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<parameters>-5 -5 -5 5 5 5</parameters>
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</space>
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</source>
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<energy_mode>multi-group</energy_mode>
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</settings>
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28
tests/test_mg_convert/results_true.dat
Normal file
28
tests/test_mg_convert/results_true.dat
Normal file
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@ -0,0 +1,28 @@
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k-combined:
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9.957263E-01 5.469041E-05
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k-combined:
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9.957263E-01 5.469041E-05
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k-combined:
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9.963652E-01 5.444550E-05
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k-combined:
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9.957263E-01 5.469041E-05
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k-combined:
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9.955157E-01 5.785520E-05
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k-combined:
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9.954023E-01 5.694553E-05
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k-combined:
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9.955722E-01 6.075634E-05
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k-combined:
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9.955692E-01 6.094480E-05
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k-combined:
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9.955154E-01 5.775805E-05
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k-combined:
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9.956787E-01 5.915112E-05
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k-combined:
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9.957022E-01 5.952369E-05
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k-combined:
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9.953517E-01 5.920431E-05
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k-combined:
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9.957263E-01 5.469041E-05
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k-combined:
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9.957263E-01 5.469041E-05
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207
tests/test_mg_convert/test_mg_convert.py
Executable file
207
tests/test_mg_convert/test_mg_convert.py
Executable file
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@ -0,0 +1,207 @@
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#!/usr/bin/env python
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import os
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import sys
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import hashlib
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sys.path.insert(0, os.pardir)
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import numpy as np
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from testing_harness import PyAPITestHarness
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import openmc
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# OpenMC simulation parameters
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batches = 2000
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inactive = 100
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particles = 1000
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def build_mgxs_library(convert):
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# Instantiate the energy group data
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groups = openmc.mgxs.EnergyGroups(group_edges=[1e-5, 0.625, 20.0e6])
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# Instantiate the 7-group (C5G7) cross section data
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uo2_xsdata = openmc.XSdata('UO2', groups)
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uo2_xsdata.order = 2
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uo2_xsdata.set_total([2., 2.])
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uo2_xsdata.set_absorption([1., 1.])
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scatter_matrix = np.array([[[0.75, 0.25],
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[0.00, 1.00]],
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[[0.75 / 3., 0.25 / 3.],
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[0.00 / 3., 1.00 / 3.]],
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[[0.75 / 4., 0.25 / 4.],
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[0.00 / 4., 1.00 / 4.]]])
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scatter_matrix = np.rollaxis(scatter_matrix, 0, 3)
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uo2_xsdata.set_scatter_matrix(scatter_matrix)
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uo2_xsdata.set_fission([0.5, 0.5])
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uo2_xsdata.set_nu_fission([1., 1.])
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uo2_xsdata.set_chi([1., 0.])
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mg_cross_sections_file = openmc.MGXSLibrary(groups)
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mg_cross_sections_file.add_xsdatas([uo2_xsdata])
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if convert is not None:
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if isinstance(convert[0], list):
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for conv in convert:
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if conv[0] in ['legendre', 'tabular', 'histogram']:
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mg_cross_sections_file = \
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mg_cross_sections_file.convert_scatter_format(
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conv[0], conv[1])
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elif conv[0] in ['angle', 'isotropic']:
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mg_cross_sections_file = \
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mg_cross_sections_file.convert_representation(
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conv[0], conv[1], conv[1])
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elif convert[0] in ['legendre', 'tabular', 'histogram']:
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mg_cross_sections_file = \
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mg_cross_sections_file.convert_scatter_format(
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convert[0], convert[1])
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elif convert[0] in ['angle', 'isotropic']:
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mg_cross_sections_file = \
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mg_cross_sections_file.convert_representation(
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convert[0], convert[1], convert[1])
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mg_cross_sections_file.export_to_hdf5()
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class MGXSTestHarness(PyAPITestHarness):
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def _build_inputs(self):
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# Instantiate some Macroscopic Data
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uo2_data = openmc.Macroscopic('UO2')
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# Instantiate some Materials and register the appropriate objects
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mat = openmc.Material(material_id=1, name='UO2 fuel')
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mat.set_density('macro', 1.0)
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mat.add_macroscopic(uo2_data)
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# Instantiate a Materials collection and export to XML
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materials_file = openmc.Materials([mat])
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materials_file.cross_sections = "./mgxs.h5"
|
||||
materials_file.export_to_xml()
|
||||
|
||||
# Instantiate ZCylinder surfaces
|
||||
left = openmc.XPlane(surface_id=4, x0=-5., name='left')
|
||||
right = openmc.XPlane(surface_id=5, x0=5., name='right')
|
||||
bottom = openmc.YPlane(surface_id=6, y0=-5., name='bottom')
|
||||
top = openmc.YPlane(surface_id=7, y0=5., name='top')
|
||||
|
||||
left.boundary_type = 'reflective'
|
||||
right.boundary_type = 'vacuum'
|
||||
top.boundary_type = 'reflective'
|
||||
bottom.boundary_type = 'reflective'
|
||||
|
||||
# Instantiate Cells
|
||||
fuel = openmc.Cell(cell_id=1, name='cell 1')
|
||||
|
||||
# Use surface half-spaces to define regions
|
||||
fuel.region = +left & -right & +bottom & -top
|
||||
|
||||
# Register Materials with Cells
|
||||
fuel.fill = mat
|
||||
|
||||
# Instantiate Universe
|
||||
root = openmc.Universe(universe_id=0, name='root universe')
|
||||
|
||||
# Register Cells with Universe
|
||||
root.add_cells([fuel])
|
||||
|
||||
# Instantiate a Geometry, register the root Universe, and export to XML
|
||||
geometry = openmc.Geometry(root)
|
||||
geometry.export_to_xml()
|
||||
|
||||
settings_file = openmc.Settings()
|
||||
settings_file.energy_mode = "multi-group"
|
||||
settings_file.batches = batches
|
||||
settings_file.inactive = inactive
|
||||
settings_file.particles = particles
|
||||
|
||||
# Create an initial uniform spatial source distribution
|
||||
bounds = [-5, -5, -5, 5, 5, 5]
|
||||
uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:])
|
||||
settings_file.source = openmc.source.Source(space=uniform_dist)
|
||||
|
||||
settings_file.export_to_xml()
|
||||
|
||||
def _run_openmc(self):
|
||||
# Run multiple conversions to compare results
|
||||
cases = [None, ['legendre', 2], ['legendre', 0],
|
||||
['tabular', 33], ['histogram', 32],
|
||||
[['tabular', 33], ['legendre', 1]],
|
||||
[['tabular', 33], ['tabular', 3]],
|
||||
[['tabular', 33], ['histogram', 32]],
|
||||
[['histogram', 32], ['legendre', 1]],
|
||||
[['histogram', 32], ['tabular', 3]],
|
||||
[['histogram', 32], ['histogram', 16]],
|
||||
[['histogram', 32], ['histogram', 128]],
|
||||
['angle', 2], [['angle', 2], ['isotropic', None]]]
|
||||
|
||||
outstr = ''
|
||||
for case in cases:
|
||||
build_mgxs_library(case)
|
||||
|
||||
if self._opts.mpi_exec is not None:
|
||||
returncode = openmc.run(mpi_procs=self._opts.mpi_np,
|
||||
openmc_exec=self._opts.exe,
|
||||
mpi_exec=self._opts.mpi_exec)
|
||||
|
||||
else:
|
||||
returncode = openmc.run(openmc_exec=self._opts.exe)
|
||||
|
||||
assert returncode == 0, 'OpenMC did not exit successfully.'
|
||||
|
||||
sp = openmc.StatePoint('statepoint.' + str(batches) + '.h5')
|
||||
|
||||
# Write out k-combined.
|
||||
outstr += 'k-combined:\n'
|
||||
form = '{0:12.6E} {1:12.6E}\n'
|
||||
outstr += form.format(sp.k_combined[0], sp.k_combined[1])
|
||||
sp.close()
|
||||
|
||||
return outstr
|
||||
|
||||
def _get_results(self, outstr, hash_output=False):
|
||||
# Hash the results if necessary.
|
||||
if hash_output:
|
||||
sha512 = hashlib.sha512()
|
||||
sha512.update(outstr.encode('utf-8'))
|
||||
outstr = sha512.hexdigest()
|
||||
|
||||
return outstr
|
||||
|
||||
def _cleanup(self):
|
||||
super(MGXSTestHarness, self)._cleanup()
|
||||
f = os.path.join(os.getcwd(), 'mgxs.h5')
|
||||
if os.path.exists(f):
|
||||
os.remove(f)
|
||||
|
||||
def execute_test(self):
|
||||
"""Build input XMLs, run OpenMC, and verify correct results."""
|
||||
try:
|
||||
self._build_inputs()
|
||||
inputs = self._get_inputs()
|
||||
self._write_inputs(inputs)
|
||||
self._compare_inputs()
|
||||
outstr = self._run_openmc()
|
||||
results = self._get_results(outstr)
|
||||
self._write_results(results)
|
||||
self._compare_results()
|
||||
finally:
|
||||
self._cleanup()
|
||||
|
||||
def update_results(self):
|
||||
"""Update results_true.dat and inputs_true.dat"""
|
||||
try:
|
||||
self._build_inputs()
|
||||
inputs = self._get_inputs()
|
||||
self._write_inputs(inputs)
|
||||
self._overwrite_inputs()
|
||||
outstr = self._run_openmc()
|
||||
results = self._get_results(outstr)
|
||||
self._write_results(results)
|
||||
self._overwrite_results()
|
||||
finally:
|
||||
self._cleanup()
|
||||
|
||||
|
||||
if __name__ == '__main__':
|
||||
harness = MGXSTestHarness('statepoint.10.*', False)
|
||||
harness.main()
|
||||
Loading…
Add table
Add a link
Reference in a new issue