openmc.CMFDMesh¶
-
class
openmc.
CMFDMesh
[source]¶ A structured Cartesian mesh used for Coarse Mesh Finite Difference (CMFD) acceleration.
Variables: - lower_left (Iterable of float) – The lower-left corner of the structured mesh. If only two coordinates are given, it is assumed that the mesh is an x-y mesh.
- upper_right (Iterable of float) – The upper-right corner of the structrued mesh. If only two coordinates are given, it is assumed that the mesh is an x-y mesh.
- dimension (Iterable of int) – The number of mesh cells in each direction.
- width (Iterable of float) – The width of mesh cells in each direction.
- energy (Iterable of float) – Energy bins in eV, listed in ascending order (e.g. [0.0, 0.625e-1, 20.0e6]) for CMFD tallies and acceleration. If no energy bins are listed, OpenMC automatically assumes a one energy group calculation over the entire energy range.
- albedo (Iterable of float) – Surface ratio of incoming to outgoing partial currents on global boundary conditions. They are listed in the following order: -x +x -y +y -z +z.
- map (Iterable of int) –
An optional acceleration map can be specified to overlay on the coarse mesh spatial grid. If this option is used, a
1
is used for a non-accelerated region and a2
is used for an accelerated region. For a simple 4x4 coarse mesh with a 2x2 fuel lattice surrounded by reflector, the map is:[1, 1, 1, 1, 1, 2, 2, 1, 1, 2, 2, 1, 1, 1, 1, 1]
Therefore a 2x2 system of equations is solved rather than a 4x4. This is extremely important to use in reflectors as neutrons will not contribute to any tallies far away from fission source neutron regions. A
2
must be used to identify any fission source region.