Handling consistency in solutionControls class

Note: additional machinery to enable easy top-level calls for
time/under-relaxation consistency in segregated solution algorithms.
Does not compile: still missing functions in ddtSchemes
This commit is contained in:
Vuko Vukcevic 2016-12-23 14:53:52 +01:00
parent 9259021903
commit 1acf0274ce
3 changed files with 297 additions and 10 deletions

View file

@ -60,6 +60,9 @@ int main(int argc, char *argv[])
# include "CourantNo.H" # include "CourantNo.H"
// Time-derivative matrix
fvVectorMatrix ddtUEqn(fvm::ddt(U));
// Convection-diffusion matrix // Convection-diffusion matrix
fvVectorMatrix HUEqn fvVectorMatrix HUEqn
( (
@ -69,7 +72,7 @@ int main(int argc, char *argv[])
if (piso.momentumPredictor()) if (piso.momentumPredictor())
{ {
solve(fvm::ddt(U) + HUEqn == -fvc::grad(p)); solve(ddtUEqn + HUEqn == -fvc::grad(p));
} }
// Prepare clean 1/a_p without time derivative contribution // Prepare clean 1/a_p without time derivative contribution
@ -81,9 +84,9 @@ int main(int argc, char *argv[])
{ {
// Calculate U from convection-diffusion matrix // Calculate U from convection-diffusion matrix
U = rAU*HUEqn.H(); U = rAU*HUEqn.H();
// Consistently calculate flux and face velocity // Consistently calculate flux
phi = piso.timeConsistentFlux(U, rAU); piso.calculateTimeConsistentFlux(phi, U, rAU);
adjustPhi(phi, U, p); adjustPhi(phi, U, p);
@ -91,7 +94,14 @@ int main(int argc, char *argv[])
{ {
fvScalarMatrix pEqn fvScalarMatrix pEqn
( (
fvm::laplacian(rAU, p) == fvc::div(phi) fvm::laplacian
(
rAU/fvc::interpolate(piso.aCoeff()),
p,
"laplacian(rAU," + p.name() + ')'
)
==
fvc::div(phi)
); );
pEqn.setReference(pRefCell, pRefValue); pEqn.setReference(pRefCell, pRefValue);
@ -109,8 +119,7 @@ int main(int argc, char *argv[])
# include "continuityErrs.H" # include "continuityErrs.H"
// Consistently reconstruct velocity after pressure equation // Consistently reconstruct velocity after pressure equation
U = piso.timeConsistentVelocity(U, rAU, p); piso.reconstructVelocity(U, ddtUEqn, rAU, p, phi);
U.correctBoundaryConditions();
} }
runTime.write(); runTime.write();

View file

@ -25,6 +25,7 @@ License
#include "solutionControl.H" #include "solutionControl.H"
#include "lduMatrix.H" #include "lduMatrix.H"
#include "demandDrivenData.H"
// * * * * * * * * * * * * * * Static Data Members * * * * * * * * * * * * * // // * * * * * * * * * * * * * * Static Data Members * * * * * * * * * * * * * //
@ -236,14 +237,244 @@ Foam::solutionControl::solutionControl(fvMesh& mesh, const word& algorithmName)
transonic_(false), transonic_(false),
consistent_(false), consistent_(false),
corr_(0), corr_(0),
corrNonOrtho_(0) corrNonOrtho_(0),
aCoeffPtr_(NULL),
faceUPtr_(NULL)
{} {}
// * * * * * * * * * * * * * * * * Destructor * * * * * * * * * * * * * * * // // * * * * * * * * * * * * * * * * Destructor * * * * * * * * * * * * * * * //
Foam::solutionControl::~solutionControl() Foam::solutionControl::~solutionControl()
{} {
deleteDemandDrivenData(aCoeffPtr_);
deleteDemandDrivenData(faceUPtr_);
}
// * * * * * * * * * * * * * * * Member Functions * * * * * * * * * * * * * //
void Foam::solutionControl::calcTimeConsistentFlux
(
surfaceScalarField& phi,
const volVectorField& U,
const volScalarField& rAU
)
{
// Store necessary fields for time consistency if they are not present
if (!aCoeffPtr_ && !faceUPtr_)
{
aCoeffPtr_ = new volScalarField
(
IOobject
(
"aCoeff",
mesh_.time().timeName(),
mesh_,
IOobject::NO_READ,
IOobject::NO_WRITE
),
mesh_,
dimensionedScalar("zero", dimless, 0.0)
);
faceUPtr_ = new surfaceVectorField
(
IOobject
(
"faceU",
mesh_.time().timeName(),
mesh_,
IOobject::NO_READ,
IOobject::NO_WRITE
),
mesh_,
dimensionedScalar("zero", dimVelocity, 0.0)
);
}
else if (!aCoeffPtr_ || !faceUPtr_)
{
FatalErrorIn
(
"tmp<surfaceScalarField> solutionControl::timeConsistentFlux"
"\n("
"\n const volVectorField& U,"
"\n const volScalarField& rAU"
"\n)"
) << "Either aCoeffPtr_ or faceUPtr_ is allocated while the"
<< " other is not. This must not happen."
<< endl
<< exit(FatalError);
}
// Now that we are sure that pointers are valid and the fields are there, we
// can do the calculation of the flux, while storing necessary data for
// future velocity reconstruction.
// Algorithm:
// 1. Update flux and aCoeff due to ddt discretisation
// 2. Update flux and aCoeff due to under-relaxation
// 3. Scale the flux with aCoeff, making sure that flux at fixed boundaries
// remains is consistent
// Get fields that will be updated
volScalarField& aCoeff = *aCoeffPtr_;
surfaceVectorField& faceU = *faceUPtr_;
// Update face interpolated velocity field. Note: handling of oldTime faceU
// fields happens in ddt scheme when calling ddtConsistentPhiCorr
faceU = fvc::interpolate(U);
// Interpolate original rAU on the faces
const surfaceScalarField rAUf = fvc::interpolate(rAU);
// Calculate the ordinary part of the flux (H/A)
phi = (faceU & mesh_.Sf());
// STAGE 1: consistent ddt discretisation handling
// Add consistent flux contribution due to ddt discretisation
phi += fvc::ddtConsistentPhiCorr(U, rAUf, faceU);
// Reset aCoeff according to ddt discretisation
aCoeff = fvc::ddtRAUCorr(U, rAU); // Note: returns 1 + ddt(U).A()*rAU
// STAGE 2: consistent under-relaxation handling
// Get under-relaxation factor used in this iteration
const dimensionedScalar alphaU
(
"alphaU",
dimless,
mesh_.solutionDict().equationRelaxationFactor
(
U.select(this->finalIter())
)
);
// Helper variable
const dimensionedScalar urfCoeff = (1.0 - alphaU)/alphaU;
// Add consistent flux contribution due to possible under-relaxation
phi += urfCoeff*fvc::interpolate(aCoeff)*phi.prevIter();
// Add under-relaxation contribution to aCoeff
aCoeff += urfCoeff*aCoeff;
// Note: this is not 100% entirely consistent with the way FOAM handles
// under-relaxation. In fvMatrix::relax() member function, the diagonal
// dominance is first assured by limiting the diagonal and the matrix is
// then relaxed. However, this is a very minor inconsistency, especially
// since this term vanishes when non-linear iterations converge to a tight
// tolerance (achieving steady state in SIMPLE or converging PISO/PIMPLE in
// each time step). VV, 23/Dec/2016.
// STAGE 3: scale the flux and correct it at the boundaries
// Scale the flux
phi /= fvc::interpolate(aCoeff);
// Get necessary data
const volVectorField::GeometricBoundaryField& Ub = U.boundaryField();
const surfaceVectorField::GeometricBoundaryField& Sb =
mesh_.Sf().boundaryField();
surfaceScalarField::GeometricBoundaryField& phib = phi.boundaryField();
// Correct flux at boundaries depending on patch type. Note: it is possible
// that we missed some important boundary conditions that need special
// considerations when calculating the flux. Maybe we can reorganise this in
// future by relying on distinction between = and == operators for
// fvsPatchFields. However, that would require serious changes at the
// moment. VV, 23/Dec/2016.
forAll (phib, patchI)
{
if (Ub[patchI].fixesValue())
{
// This is fixed value patch, flux needs to be recalculated
// respecting the boundary condition
phib[patchI] == (Ub[patchI] & Sb[patchI]);
}
else if
(
isA<slipFvPatchVectorField>(Ub[patchI])
|| isA<symmetryFvPatchVectorField>(Ub[patchI]])
)
{
// This is slip or symmetry, flux needs to be zero
phib[patchI] == 0.0;
}
}
}
void Foam::solutionControl::reconstructVelocity
(
volVectorField& U,
const fvVectorMatrix& ddtUEqn,
const volScalarField& rAU,
const volScalarField& p,
const surfaceScalarField& phi
)
{
// Reconstruct the velocity using all the components from original equation
U = 1.0/(1.0/rAU + ddtUEqn.A())*
(
U/rAU + ddtUEqn.H() - fvc::grad(p)
);
U.correctBoundaryConditions();
// Update divergence free face velocity field, whose value will be used in
// the next time step
if (!faceUPtr_)
{
FatalErrorIn
(
"void solutionControl::reconstructVelocity"
"\n("
"\n volVectorField& U,"
"\n const volVectorField& ddtUEqn,"
"\n const volScalarField& rAU,"
"\n const volScalarField& p"
"\n) const"
) << "faceUPtr_ not calculated. Make sure you have called"
<< " calculateTimeConsistentFlux(...) before calling this function."
<< endl;
<< exit(FatalError);
}
surfaceVectorField& faceU = *faceUPtr_;
// First interpolate the reconstructed velocity on the faces
faceU = fvc::interpolate(U);
// Replace the normal component with conservative flux
const surfaceVectorField& Sf = mesh_.Sf();
const surfaceVectorField rSf = Sf/magSqr(Sf);
// Subtract interpolated normal component
faceU -= (Sf & faceU)*rSf;
// Now that the normal component is zero, add the normal component from
// conservative flux
faceU += phi*rSf;
}
const Foam::volScalarField& Foam::solutionControl::aCoeff() const
{
if (!aCoeffPtr_)
{
FatalErrorIn
(
"const volScalarField& solutionControl::aCoeff() const"
) << "aCoeffPtr_ not calculated. Make sure you have called"
<< " calculateTimeConsistentFlux(...) before calling aCoeff()."
<< endl;
<< exit(FatalError);
}
return *aCoeffPtr_;
}
// ************************************************************************* // // ************************************************************************* //

View file

@ -25,7 +25,9 @@ Class
Foam::solutionControl Foam::solutionControl
Description Description
Base class for solution control classes Base class for solution control classes.
The class also provides additional member functions for calculation
of time and under-relaxation consistent flux and velocity.
\*---------------------------------------------------------------------------*/ \*---------------------------------------------------------------------------*/
@ -145,6 +147,19 @@ protected:
private: private:
// Private data
// Fields necessary for time and under-relaxation consistency
//- A coeff (A^~) arising from consistency formulation
volScalarField* aCoeffPtr_;
//- Face velocity needed for consistent formulation
surfaceVectorField* faceUPtr_;
// Private member functions
//- Disallow default bitwise copy construct //- Disallow default bitwise copy construct
solutionControl(const solutionControl&); solutionControl(const solutionControl&);
@ -204,6 +219,38 @@ public:
inline bool consistent() const; inline bool consistent() const;
// Time and under-relaxation consistency. Note: these functions could be
// made virtual and specific to SIMPLE, PISO and PIMPLE, but we will
// make them general in sense they account for arbitrary ddt scheme
// and arbitrary under-relaxation (e.g. if someone runs SIMPLE in
// transient mode or PISO with under-relaxation)
//- Calculate and return time consistent flux (before pressure
// equation). At point of call, U = H/A where H and A come from
// convection-diffusion equation only.
void calculateTimeConsistentFlux
(
surfaceScalarField& phi,
const volVectorField& U,
const volScalarField& rAU
);
//- Reconstruct velocity (after pressure equation). At point of
// call, U = H/A where H and A come from convection-diffusion
// equation only
void reconstructVelocity
(
volVectorField& U,
const fvVectorMatrix& ddtUEqn,
const volScalarField& rAU,
const volScalarField& p,
const surfaceScalarField& phi
);
//- Const access to aCoeff (needed for pressure equation)
const volScalarField& aCoeff() const;
// Evolution // Evolution
//- Main control loop //- Main control loop