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flow 1.3.0
Kokkos cut-cell IBM incompressible Navier-Stokes solver + pnm pore extraction
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#include <flow_ibm.hpp>
Public Attributes | |
| double | mdotMin = 0.0 |
| double | mdotMax = 0.0 |
| double | mdotMean = 0.0 |
| long | interfaceCells = 0 |
| double | removedVolume = 0.0 |
| sum of dV actually subtracted this step (+ = evaporated) | |
| double | redistributed = 0.0 |
| |clip deficit| pushed into neighbours this step | |
| long | deficitCells = 0 |
| cells that clipped at C = 0 | |
| long | excessCells = 0 |
| cells that clipped at C = 1 | |
| double | sourceSum = 0.0 |
| sum of the deposited divergence source over inner cells (1/s) | |
| long | sourceCells = 0 |
| cells that RECEIVED a deposit | |
| long | fallbackCells = 0 |
| interfacial cells whose +n walk found no pure gas cell | |
| double | unresolved = 0.0 |
| clip residue no neighbour could absorb (pushed anyway) | |
| double | minC = 0.0 |
| double | maxC = 0.0 |
| double | area = 0.0 |
| sum of the PLIC polygon areas over interfacial cells (h^2) | |
| double | bandDiv = 0.0 |
| max |div(open u)| over interfacial cells (WO-P23; see pcBandDivergence) | |
| double | Tmin = 0.0 |
| double | Tmax = 0.0 |
| energy-scalar extrema (consistent transport only) | |
| long | areaHf = 0 |
| WO-P3c: cells whose area came from a height function (tiers 1/2a) | |
| long | areaPv = 0 |
| WO-P3c: cells whose area came from the PV paraboloid (tier 3) | |
| long | areaNone = 0 |
| WO-P3c: cells with NO cascade geometry (kept their MYC PLIC area) | |
| double | areaOrphan = 0.0 |
| WO-P3d: area the JOINED sheet booked to cells that are not interfacial, i.e. | |
| double | mdotFit = 0.0 |
| WO-P3g: the AREA-WEIGHTED one-sided-fit mdot, kept as the diagnostic that item 1 replaced (0 unless the operator flux is on) | |
| double | qOperator = 0.0 |
| WO-P3g: the heat (W) the operator's Dirichlet rows draw across the interface, i.e. | |
| double | qOrphan = 0.0 |
| ... the part of it on interfacial cells with NO area, which the regression drops: the ONE non-conservation item 1 cannot remove | |
Definition at line 3943 of file flow_ibm.hpp.
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::mdotMin = 0.0 |
Definition at line 3944 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::mdotMax = 0.0 |
Definition at line 3944 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::mdotMean = 0.0 |
Definition at line 3944 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::interfaceCells = 0 |
Definition at line 3945 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::removedVolume = 0.0 |
sum of dV actually subtracted this step (+ = evaporated)
Definition at line 3946 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcRegress().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::redistributed = 0.0 |
|clip deficit| pushed into neighbours this step
Definition at line 3947 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcRegress().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::deficitCells = 0 |
cells that clipped at C = 0
Definition at line 3948 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcRegress().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::excessCells = 0 |
cells that clipped at C = 1
Definition at line 3949 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcRegress().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::sourceSum = 0.0 |
sum of the deposited divergence source over inner cells (1/s)
Definition at line 3950 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcScatterSource().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::sourceCells = 0 |
cells that RECEIVED a deposit
Definition at line 3951 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcScatterSource().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::fallbackCells = 0 |
interfacial cells whose +n walk found no pure gas cell
Definition at line 3952 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::unresolved = 0.0 |
clip residue no neighbour could absorb (pushed anyway)
Definition at line 3953 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcRegress().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::minC = 0.0 |
Definition at line 3954 of file flow_ibm.hpp.
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::maxC = 0.0 |
Definition at line 3954 of file flow_ibm.hpp.
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::area = 0.0 |
sum of the PLIC polygon areas over interfacial cells (h^2)
Definition at line 3955 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::bandDiv = 0.0 |
max |div(open u)| over interfacial cells (WO-P23; see pcBandDivergence)
Definition at line 3956 of file flow_ibm.hpp.
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::Tmin = 0.0 |
Definition at line 3957 of file flow_ibm.hpp.
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::Tmax = 0.0 |
energy-scalar extrema (consistent transport only)
Definition at line 3957 of file flow_ibm.hpp.
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::areaHf = 0 |
WO-P3c: cells whose area came from a height function (tiers 1/2a)
Definition at line 3958 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::areaPv = 0 |
WO-P3c: cells whose area came from the PV paraboloid (tier 3)
Definition at line 3959 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| long peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::areaNone = 0 |
WO-P3c: cells with NO cascade geometry (kept their MYC PLIC area)
Definition at line 3960 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::areaOrphan = 0.0 |
WO-P3d: area the JOINED sheet booked to cells that are not interfacial, i.e.
the part of the sum the flux integral drops
Definition at line 3961 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::mdotFit = 0.0 |
WO-P3g: the AREA-WEIGHTED one-sided-fit mdot, kept as the diagnostic that item 1 replaced (0 unless the operator flux is on)
Definition at line 3963 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::qOperator = 0.0 |
WO-P3g: the heat (W) the operator's Dirichlet rows draw across the interface, i.e.
sum mdot A h_lv by construction
Definition at line 3965 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().
| double peclet::flow::Solver< Grid >::PhaseChangeDiagnostics::qOrphan = 0.0 |
... the part of it on interfacial cells with NO area, which the regression drops: the ONE non-conservation item 1 cannot remove
Definition at line 3967 of file flow_ibm.hpp.
Referenced by peclet::flow::Solver< Grid >::pcBuildInterface().