armi.physics.neutronics.latticePhysics.latticePhysicsInterface module

” Lattice Physics Interface.

Parent classes for codes responsible for generating broad-group cross sections

armi.physics.neutronics.latticePhysics.latticePhysicsInterface.setBlockNeutronVelocities(r, neutronVelocities)[source]

Set the mgNeutronVelocity parameter for each block using the neutronVelocities dictionary data.

Parameters:

neutronVelocities (dict) – Dictionary that is keyed with the representativeBlock XS IDs with values of multigroup neutron velocity data computed by MC2.

Raises:

ValueError – Multi-group neutron velocities was not computed during the cross section calculation.

class armi.physics.neutronics.latticePhysics.latticePhysicsInterface.LatticePhysicsInterface(r, cs)[source]

Bases: Interface

Class for interacting with lattice physics codes.

function = 'latticePhysics'

The function performed by an Interface. This is not required be be defined by implementations of Interface, but is used to form categories of interfaces.

interactBOL(cycle=0)[source]

Run the lattice physics code if genXS is set and update burnup groups.

Generate new cross sections based off the case settings and the current state of the reactor if the lattice physics frequency is BOL.

interactBOC(cycle=0)[source]

Run the lattice physics code if genXS is set and update burnup groups.

Generate new cross sections based off the case settings and the current state of the reactor if the lattice physics frequency is BOC.

Notes

armi.physics.fuelCycle.fuelHandlerInterface.FuelHandlerInterface.interactBOC() also calls this if the ``runLatticePhysicsBeforeShuffling``setting is True. This happens because branch searches may need XS.

updateXSLibrary(cycle, node=None)[source]

Update the current XS library, either by creating or reloading one.

Parameters:
  • cycle (int) – The cycle that is being processed. Used to name the library.

  • node (int, optional) – The node that is being processed. Used to name the library.

See also

computeCrossSections

run lattice physics on the current reactor state no matter weather needed or not.

readExistingXSLibraries(cycle, node)[source]
makeCycleXSFilesAsBaseFiles(cycle, node)[source]
interactEveryNode(cycle=None, node=None)[source]

Run the lattice physics code if genXS is set and update burnup groups.

Generate new cross sections based off the case settings and the current state of the reactor if the lattice physics frequency is at least everyNode.

interactCoupled(iteration)[source]

Runs on coupled iterations to generate cross sections that are updated with the temperature state.

Notes

This accounts for changes in cross section data due to temperature changes, which are important for cross section resonance effects and accurately characterizing Doppler constant and coefficient evaluations. For Standard and Equilibrium run types, this coupling iteration is limited to when the time node is equal to zero. The validity of this assumption lies in the expectation that these runs have consistent power, flow, and temperature conditions at all time nodes. For Snapshot run types, this assumption, in general, is invalidated as the requested reactor state may sufficiently differ from what exists on the database and where tight coupling is needed to capture temperature effects.

Warning

For Standard and Equilibrium run types, if the reactor power, flow, and/or temperature state is expected to vary over the lifetime of the simulation, as could be the case with detailed cycle histories, a custom subclass should be considered.

Parameters:

iteration (int) – This is unused since cross sections are generated on a per-cycle basis.

clearXS()[source]
interactEOC(cycle=None)[source]

Interact at the end of a cycle.

Force updating cross sections at the start of the next cycle.

computeCrossSections(baseList=None, forceSerial=False, xsLibrarySuffix='', blockList=None)[source]

Prepare a batch of inputs, execute them, and store results on reactor library.

Parameters:
  • baseList (list) – a user-specified set of bases that will be run instead of calculating all of them

  • forceSerial (bool, optional) – Will run on 1 processor in sequence instead of on many in parallel Useful for optimization/batch runs where every processor is on a different branch

  • xsLibrarySuffix (str, optional) – A book-keeping suffix used in Doppler calculations

  • blockList (list, optional) – List of blocks for which to generate cross sections. If None, representative blocks will be determined

generateLatticePhysicsInputs(baseList, xsLibrarySuffix, blockList, xsWriters=None)[source]

Write input files for the generation of cross section libraries.

Parameters:
  • baseList (list) – A list of cross-section id strings (e.g. AA, BC) that will be generated. Default: all in reactor

  • xsLibrarySuffix (str) – A suffix added to the end of the XS file names such as ‘voided’ for voided XS. Default: Empty

  • blockList (list) – The blocks to write inputs for.

  • xsWriters (list, optional) – The specified writers to write the input files

Returns:

returnedFromWriters – A list of what this specific writer instance returns for each representative block. It is the responsibility of the subclassed interface to implement. In many cases, it is the executing agent.

Return type:

list

getWriters(representativeBlock, xsLibrarySuffix, writers=None)[source]

Return valid lattice physics writer subclass(es).

Parameters:
  • representativeBlock (Block) – A representative block object that can be created from a block collection.

  • xsLibrarySuffix (str) – A suffix added to the end of the XS file names such as ‘voided’ for voided XS. Default: Empty

  • writers (list of lattice physics writer objects, optional) – If the writers are known, they can be provided and constructed.

Returns:

writers – A list of writers for the provided representative block.

Return type:

list

getReader()[source]
getRepresentativeBlocks()[source]

Return a list of all blocks in the problem.

updatePhysicsCouplingControl()[source]

Disable XS update in equilibrium cases after a while.

Notes

This is only relevant for equilibrium cases. We have to turn off XS updates after several cyclics or else the number densities will never converge.