compressible::alphatWallBoilingWallFunction: Improved solution procedure
This boundary condition now solves for the wall temperature by interval
bisection, which should be significantly more robust than the previous
fixed-point iteration procedure. There is a new non-dimensional
"tolerance" setting that controls how tightly this solution procedure
solves the wall temperature. The "relax" setting is no longer used.
The boundary condition no longer triggers re-evaluation of the
temperature condition in order to re-calculate the heat flux within the
solution iteration. Instead, it extracts physical coefficients from the
form of the boundary condition and uses these to form a linearised
approximation of the heat flux. This is a more general approach, and
will not trigger side-effects associated with re-evaluating the
temperature condition.
The fixedMultiphaseHeatFlux condition has been replaced by a
uniformFixedMultiphaseHeatFlux condition, which constructs a mixed
constraint which portions a specified heat flux between the phases in
such a way as to keep the boundary temperature uniform across all
phases. This can be applied to all phases. It is no longer necessary to
apply a heat flux model to one "master" phase, then map the resulting
temperature to the others. An example specification of this boundary
condition is as follows:
wall
{
type uniformFixedMultiphaseHeatFlux;
q 1000;
relax 0.3;
value $internalField;
}
The wall boiling tutorials have been updated to use these new functions,
and time-varying heat input has been used to replace the
stop-modify-restart pattern present in the single-region cases.
This commit is contained in:
@ -35,13 +35,10 @@ boundaryField
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otherPhase liquid;
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phaseType vapor;
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Prt 0.85;
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Cmu 0.09;
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kappa 0.41;
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E 9.8;
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partitioningModel
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{
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type Lavieville;
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alphaCrit 0.2;
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type Lavieville;
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alphaCrit 0.2;
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}
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value uniform 0;
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}
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@ -32,31 +32,27 @@ boundaryField
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wall
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{
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type compressible::alphatWallBoilingWallFunction;
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Prt 0.85;
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Cmu 0.09;
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kappa 0.41;
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E 9.8;
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relax 1.0;
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otherPhase gas;
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phaseType liquid;
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Prt 0.85;
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partitioningModel
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{
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type Lavieville;
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alphaCrit 0.2;
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type Lavieville;
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alphaCrit 0.2;
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}
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nucleationSiteModel
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{
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type LemmertChawla;
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Cn 1;
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NRef 30000000;
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deltaTRef 10;
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type LemmertChawla;
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Cn 1;
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NRef 30000000;
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deltaTRef 10;
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}
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departureDiamModel
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{
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type TolubinskiKostanchuk;
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dRef 0.00024;
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dMax 0.0014;
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dMin 1e-06;
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type TolubinskiKostanchuk;
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dRef 0.00024;
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dMax 0.0014;
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dMin 1e-06;
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}
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departureFreqModel
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{
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@ -7,7 +7,7 @@ cd ${0%/*} || exit 1 # run from this directory
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runApplication blockMesh
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runApplication extrudeMesh
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runApplication splitMeshRegions -cellZones -overwrite
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runApplication foamDictionary constant/fluid/polyMesh/boundary -entry entry0/inlet/neighbourRegion -set "fluid"
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paraFoam -region fluid -touch
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paraFoam -region solid -touch
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@ -16,6 +16,7 @@ runApplication decomposePar -allRegions
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runParallel $(getApplication)
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runApplication reconstructPar -latestTime -allRegions
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runApplication foamPostProcess -latestTime -region fluid -func "
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graphCell
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(
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@ -24,9 +25,6 @@ runApplication foamPostProcess -latestTime -region fluid -func "
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end=(3.4901 0.0096 0),
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fields=(alpha.gas T.liquid T.gas)
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)"
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./validation/createGraphs
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runApplication -append foamPostProcess -region fluid -latestTime -func "
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patchSurface
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(
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@ -37,6 +35,10 @@ runApplication -append foamPostProcess -region fluid -latestTime -func "
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fields=(dDeparture.liquid fDeparture.liquid nucleationSiteDensity.liquid wetFraction.liquid qQuenching.liquid qEvaporative.liquid)
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)"
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./validation/createWallBoilingPropertiesGraphs
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if ! isTest "$@"
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then
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./validation/createGraphs
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./validation/createWallBoilingPropertiesGraphs
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fi
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#------------------------------------------------------------------------------
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