Merge branch 'bugfix/missingMovingMeshTreatmentInConsistency' into CumulativeDevelopment-VukoVukcevic
This commit is contained in:
commit
bf2e1cdc86
10 changed files with 206 additions and 23 deletions
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@ -660,7 +660,35 @@ CoEulerDdtScheme<Type>::fvcDdtConsistentPhiCorr
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const surfaceScalarField& rAUf
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)
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{
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return (mesh().Sf() & faceU.oldTime())*rAUf*CofrDeltaT();
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tmp<fluxFieldType> toldTimeFlux =
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(mesh().Sf() & faceU.oldTime())*rAUf*CofrDeltaT();
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes
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volScalarField V0ByV
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(
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct the flux with interpolated volume ratio
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toldTimeFlux() *= fvc::interpolate(V0ByV);
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}
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return toldTimeFlux;
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}
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@ -1201,16 +1201,39 @@ CrankNicolsonDdtScheme<Type>::fvcDdtConsistentPhiCorr
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- offCentre_(faceUDdt0())
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);
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}
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// Calculate old time flux
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fluxFieldType oldTimeFlux =
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rAUf*rDtCoef_(faceUDdt0)*(mesh().Sf() & faceU.oldTime());
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes
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volScalarField V0ByV
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(
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct the flux with interpolated volume ratio
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oldTimeFlux *= fvc::interpolate(V0ByV);
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}
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return
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rAUf*
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(
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mesh().Sf()
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& (
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rDtCoef_(faceUDdt0)*faceU.oldTime()
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+ offCentre_(faceUDdt0())
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)
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);
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oldTimeFlux
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+ rAUf*rDtCoef_(faceUDdt0)*(mesh().Sf() & offCentre_(faceUDdt0()));
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}
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@ -522,7 +522,35 @@ EulerDdtScheme<Type>::fvcDdtConsistentPhiCorr
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const surfaceScalarField& rAUf
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)
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{
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return (mesh().Sf() & faceU.oldTime())*rAUf/mesh().time().deltaT();
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tmp<fluxFieldType> toldTimeFlux =
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(mesh().Sf() & faceU.oldTime())*rAUf/mesh().time().deltaT();
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes
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volScalarField V0ByV
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(
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct the flux with interpolated volume ratio
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toldTimeFlux() *= fvc::interpolate(V0ByV);
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}
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return toldTimeFlux;
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}
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@ -665,7 +665,35 @@ SLTSDdtScheme<Type>::fvcDdtConsistentPhiCorr
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const surfaceScalarField& rAUf
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)
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{
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return (mesh().Sf() & faceU.oldTime())*rAUf*fvc::interpolate(SLrDeltaT());
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tmp<fluxFieldType> toldTimeFlux =
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(mesh().Sf() & faceU.oldTime())*rAUf*fvc::interpolate(SLrDeltaT());
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes
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volScalarField V0ByV
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(
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct the flux with interpolated volume ratio
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toldTimeFlux() *= fvc::interpolate(V0ByV);
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}
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return toldTimeFlux;
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}
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@ -732,18 +732,66 @@ backwardDdtScheme<Type>::fvcDdtConsistentPhiCorr
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const scalar rDeltaT = 1.0/deltaT;
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// Note: minus sign in gamma coefficient so we can simply add the fluxes
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// together at the end
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const dimensionedScalar beta("beta", dimless/dimTime, coefft0*rDeltaT);
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const dimensionedScalar gamma("gamma", dimless/dimTime, -coefft00*rDeltaT);
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return
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rAUf*
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// Calculate old and old-old flux contributions
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fluxFieldType oldTimeFlux =
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beta*rAUf*(mesh().Sf() & faceU.oldTime());
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fluxFieldType oldOldTimeFlux =
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gamma*rAUf*(mesh().Sf() & faceU.oldTime().oldTime());
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes for old flux contribution
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volScalarField V0ByV
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(
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mesh().Sf()
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& (
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beta*faceU.oldTime()
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+ gamma*faceU.oldTime().oldTime()
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)
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct old time flux contribution
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oldTimeFlux *= fvc::interpolate(V0ByV);
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// Also need to take into account the ratio between old-old and current
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// cell volumes for old-old time flux contribution
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volScalarField V00ByV
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(
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IOobject
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(
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"V00ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V00ByV.internalField() = mesh().V00()/mesh().V();
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V00ByV.correctBoundaryConditions();
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// Correct old-old time flux contribution
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oldOldTimeFlux *= fvc::interpolate(V00ByV);
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}
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return oldTimeFlux + oldOldTimeFlux;
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}
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@ -667,7 +667,35 @@ steadyInertialDdtScheme<Type>::fvcDdtConsistentPhiCorr
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const surfaceScalarField& rAUf
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)
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{
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return (mesh().Sf() & faceU.oldTime())*rAUf*CofrDeltaT();
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tmp<fluxFieldType> toldTimeFlux =
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(mesh().Sf() & faceU.oldTime())*rAUf*CofrDeltaT();
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if (mesh().moving())
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{
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// Mesh is moving, need to take into account the ratio between old and
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// current cell volumes
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volScalarField V0ByV
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(
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IOobject
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(
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"V0ByV",
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mesh().time().timeName(),
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mesh(),
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IOobject::NO_READ,
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IOobject::NO_WRITE
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),
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mesh(),
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dimensionedScalar("one", dimless, 1.0),
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zeroGradientFvPatchScalarField::typeName
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);
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V0ByV.internalField() = mesh().V0()/mesh().V();
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V0ByV.correctBoundaryConditions();
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// Correct the flux with interpolated volume ratio
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toldTimeFlux() *= fvc::interpolate(V0ByV);
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}
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return toldTimeFlux;
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}
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@ -18,4 +18,4 @@ done
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# Print out the converged pressure for all time steps for visual check whether
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# the solution does not depend on the time step
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tail -n 1 */probes/0/p
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tail -n 1 */postProcessing/probes/0/p
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@ -5,6 +5,6 @@ simulations are performed with four different time steps spanning four orders of
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magnitude: 0.01, 0.001, 0.0001 and 0.00001 s. Tolerances for all equations are
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very small, yielding extremely small (O(1e-11)) differences in converged
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pressure field. If the differences are larger - it means that the converged
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solution is not independent to time step size.
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solution depends on the time step size.
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Author: Vuko Vukcevic, vuko.vukcevic@fsb.hr
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@ -18,4 +18,4 @@ done
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# Print out the converged pressure for all relaxation factors for visual check
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# whether the solution does not depend on the under-relaxation factors
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tail -n 1 */probes/0/p
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tail -n 1 */postProcessing/probes/0/p
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@ -9,6 +9,6 @@ simulations are performed with five different under-relaxation pairs:
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5. alphaU = 0.4, alphap = 0.6
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Tolerances for all equations are very small, yielding extremely small (O(1e-11))
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differences in converged pressure field. If the differences are larger - it
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means that the converged solution is not independent to relaxation factors.
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means that the converged solution is dependend on relaxation factors.
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Author: Vuko Vukcevic, vuko.vukcevic@fsb.hr
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