armi.physics.neutronics.globalFlux.globalFluxInterface module¶
The Global flux interface provide a base class for all neutronics tools that compute the neutron and/or photon flux.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxInterface(r, cs)[source]¶
Bases:
armi.interfaces.Interface
A general abstract interface for global flux-calculating modules.
Should be subclassed by more specific implementations.
Construct an interface.
The
r
andcs
arguments are required, but may beNone
, where appropriate for the specificInterface
implementation.- Parameters
r (Reactor) – A reactor to attach to
cs (Settings) – Settings object to use
- Raises
RuntimeError – Interfaces derived from Interface must define their name
- name: Optional[str] = 'GlobalFlux'¶
The name of the interface. This is undefined for the base class, and must be overridden by any concrete class that extends this one.
- function = 'globalFlux'¶
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.
- getHistoryParams()[source]¶
Return parameters that will be added to assembly versus time history printouts.
- interactEveryNode(cycle, node)[source]¶
Calculate flux, power, and keff for this cycle and node.
Flux, power, and keff are generally calculated at every timestep to ensure flux is up to date with the reactor state.
- interactCoupled(iteration)[source]¶
Runs during a tightly-coupled physics iteration to updated the flux and power.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxInterfaceUsingExecuters(r, cs)[source]¶
Bases:
armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxInterface
A global flux interface that makes use of the ARMI Executer system to run.
Using Executers is optional but seems to allow easy interoperability between the myriad global flux solvers in the world.
If a new global flux solver does not fit easily into the Executer pattern, then it will be best to just start from the base GlobalFluxInterface rather than trying to adjust the Executer pattern to fit.
Notes
This points library users to the Executer object, which is intended to provide commonly-used structure useful for many global flux plugins.
Construct an interface.
The
r
andcs
arguments are required, but may beNone
, where appropriate for the specificInterface
implementation.- Parameters
r (Reactor) – A reactor to attach to
cs (Settings) – Settings object to use
- Raises
RuntimeError – Interfaces derived from Interface must define their name
- interactEveryNode(cycle, node)[source]¶
Calculate flux, power, and keff for this cycle and node.
Flux, power, and keff are generally calculated at every timestep to ensure flux is up to date with the reactor state.
- interactCoupled(iteration)[source]¶
Runs during a tightly-coupled physics iteration to updated the flux and power.
- static getOptionsCls()[source]¶
Get a blank options object.
Subclass this to allow generic updating of options.
- getExecuterOptions(label=None)[source]¶
Get an executer options object populated from current user settings and reactor.
If you want to set settings more deliberately (e.g. to specify a cross section library rather than use an auto-derived name), use
getOptionsCls
and build your own.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxOptions(label: Optional[str] = None)[source]¶
Bases:
armi.physics.executers.ExecutionOptions
Data structure representing common options in Global Flux Solvers
- fromUserSettings(cs)[source]¶
Map user input settings from cs to a set of specific global flux options.
This is not required; these options can alternatively be set programmatically.
- fromReactor(reactor: armi.reactor.reactors.Reactor)[source]¶
Set options from a particular reactor object.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxExecuter(options: armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxOptions, reactor)[source]¶
Bases:
armi.physics.executers.DefaultExecuter
A short-lived object that coordinates the prep, execution, and processing of a flux solve.
There are many forms of global flux solves:
Eigenvalue/Fixed source
Adjoint/real
Diffusion/PN/SN/MC
Finite difference/nodal
There are also many reasons someone might need a flux solve:
Update multigroup flux and power on reactor and compute keff
Just compute keff in a temporary perturbed state
Just compute flux and adjoint flux on a state to
There may also be some required transformations when a flux solve is done:
Add/remove edge assemblies
Apply a uniform axial mesh
There are also I/O performance complexities, including running on fast local paths and copying certain user-defined files back to the working directory on error or completion. Given all these options and possible needs for information from global flux, this class provides a unified interface to everything.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxResultMapper(r=None, externalCodeInterface=None, fName=None)[source]¶
Bases:
armi.interfaces.OutputReader
A short-lived class that maps neutronics output data to a reactor mode.
Neutronics results can come from a file or a pipe or in memory. This is always subclassed for specific neutronics runs but contains some generic methods that are universally useful for any global flux calculation. These are mostly along the lines of information that can be derived from other information, like dpa rate coming from dpa deltas and cycle length.
- clearFlux()[source]¶
Delete flux on all blocks. Needed to prevent stale flux when partially reloading.
- class armi.physics.neutronics.globalFlux.globalFluxInterface.DoseResultsMapper(depletionSeconds, options)[source]¶
Bases:
armi.physics.neutronics.globalFlux.globalFluxInterface.GlobalFluxResultMapper
Updates fluence and dpa when time shifts.
Often called after a depletion step.
Notes
We attempted to make this a set of stateless functions but the requirement of various options made it more of a data passing task than we liked. So it’s just a lightweight and ephemeral results mapper.
- apply(reactor)[source]¶
Apply the output back to a reactor state.
This provides a generic interface for the output data of anything to be applied to a reactor state. The application could involve reading text or binary output or simply parameters to appropriate values in some other data structure.
- updateFluenceAndDpa(stepTimeInSeconds, blockList=None)[source]¶
updates the fast fluence and the DPA of the blocklist
The dpa rate from the previous timestep is used to compute the dpa here.
- There are several items of interest computed here, including:
detailedDpa: The average DPA of a block
- detailedDpaPeak: The peak dpa of a block, considering axial and radial peaking
The peaking is based either on a user-provided peaking factor (computed in a pin reconstructed rotation study) or the nodal flux peaking factors
dpaPeakFromFluence: fast fluence * fluence conversion factor (old and inaccurate). Used to be dpaPeak
- Parameters
See also
updateDpaRate
updates the DPA rate used here to compute actual dpa
- updateCycleDoseParams()[source]¶
Updates reactor params based on the amount of dose (detailedDpa) accrued this cycle Params updated include:
maxDetailedDpaThisCycle dpaFullWidthHalfMax elevationOfACLP3Cycles elevationOfACLP7Cycles
These parameters are left as zeroes at BOC because no dose has been accumulated yet.
- updateLoadpadDose()[source]¶
Summarize the dose in DPA of the above-core load pad.
This sets the following reactor params:
loadPadDpaPeak : the peak dpa in any load pad
loadPadDpaAvg : the highest average dpa in any load pad
Warning
This only makes sense for cores with load pads on their assemblies.
See also
_calcLoadPadDose
computes the load pad dose
- armi.physics.neutronics.globalFlux.globalFluxInterface.computeDpaRate(mgFlux, dpaXs)[source]¶
Compute the DPA rate incurred by exposure of a certain flux spectrum
- Parameters
- Returns
dpaPerSecond – The dpa/s in this material due to this flux
- Return type
Notes
Displacements calculated by displacement XS
\[\begin{split}\text{Displacement rate} &= \phi N_{\text{HT9}} \sigma \\ &= (\#/\text{cm}^2/s) \cdot (1/cm^3) \cdot (\text{barn})\\ &= (\#/\text{cm}^5/s) \cdot \text{(barn)} * 10^{-24} \text{cm}^2/\text{barn} \\ &= \#/\text{cm}^3/s\end{split}\]DPA rate = displacement density rate / (number of atoms/cc) = dr [#/cm^3/s] / (nHT9) [1/cm^3] = flux * barn * 1e-24
\[\frac{\text{dpa}}{s} = \frac{\phi N \sigma}{N} = \phi * \sigma\]the Number density of the structural material cancels out. It’s in the macroscopic XS and in the original number of atoms.
- Raises
RuntimeError – Negative dpa rate.
- armi.physics.neutronics.globalFlux.globalFluxInterface.calcReactionRates(obj, keff, lib)[source]¶
Compute 1-group reaction rates for this object (usually a block.)
- Parameters
obj (Block) – The object to compute reaction rates on. Notionally this could be upgraded to be any kind of ArmiObject but with params defined as they are it currently is only implemented for a block.
keff (float) – The keff of the core. This is required to get the neutron production rate correct via the neutron balance statement (since nuSigF has a 1/keff term).
lib (XSLibrary) – Microscopic cross sections to use in computing the reaction rates.
Notes
Values include:
Fission
nufission
n2n
absorption
Scatter could be added as well. This function is quite slow so it is skipped for now as it is uncommonly needed.
Reaction rates are:
\[\Sigma \phi = \sum_{\text{nuclides}} \sum_{\text{energy}} \Sigma \phi\]The units of \(N \sigma \phi\) are:
[#/bn-cm] * [bn] * [#/cm^2/s] = [#/cm^3/s]
The group-averaged microscopic cross section is:
\[\sigma_g = \frac{\int_{E g}^{E_{g+1}} \phi(E) \sigma(E) dE}{\int_{E_g}^{E_{g+1}} \phi(E) dE}\]