fvOptions does not have the appropriate structure to support MRF as it is based on option selection by user-specified fields whereas MRF MUST be applied to all velocity fields in the particular solver. A consequence of the particular design choices in fvOptions made it difficult to support MRF for multiphase and it is easier to support frame-related and field related options separately. Currently the MRF functionality provided supports only rotations but the structure will be generalized to support other frame motions including linear acceleration, SRF rotation and 6DoF which will be run-time selectable.
200 lines
5.3 KiB
C
200 lines
5.3 KiB
C
/*---------------------------------------------------------------------------*\
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========= |
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\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
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\\ / O peration |
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\\ / A nd | Copyright (C) 2011-2015 OpenFOAM Foundation
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\\/ M anipulation |
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-------------------------------------------------------------------------------
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License
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This file is part of OpenFOAM.
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OpenFOAM is free software: you can redistribute it and/or modify it
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under the terms of the GNU General Public License as published by
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the Free Software Foundation, either version 3 of the License, or
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(at your option) any later version.
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OpenFOAM is distributed in the hope that it will be useful, but WITHOUT
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ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or
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FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License
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for more details.
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You should have received a copy of the GNU General Public License
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along with OpenFOAM. If not, see <http://www.gnu.org/licenses/>.
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Application
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potentialFoam
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Description
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Potential flow solver which solves for the velocity potential
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from which the flux-field is obtained and velocity field by reconstructing
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the flux.
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This application is particularly useful to generate starting fields for
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Navier-Stokes codes.
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\*---------------------------------------------------------------------------*/
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#include "fvCFD.H"
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#include "pisoControl.H"
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#include "fvIOoptionList.H"
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// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
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int main(int argc, char *argv[])
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{
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argList::addOption
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(
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"pName",
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"pName",
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"Name of the pressure field"
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);
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argList::addBoolOption
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(
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"initialiseUBCs",
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"Initialise U boundary conditions"
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);
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argList::addBoolOption
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(
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"writePhi",
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"Write the velocity potential field"
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);
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argList::addBoolOption
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(
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"writep",
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"Calculate and write the pressure field"
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);
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argList::addBoolOption
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(
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"withFunctionObjects",
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"execute functionObjects"
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);
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#include "setRootCase.H"
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#include "createTime.H"
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#include "createMesh.H"
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pisoControl potentialFlow(mesh, "potentialFlow");
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#include "createFields.H"
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#include "createMRF.H"
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#include "createFvOptions.H"
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// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
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Info<< nl << "Calculating potential flow" << endl;
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// Since solver contains no time loop it would never execute
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// function objects so do it ourselves
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runTime.functionObjects().start();
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MRF.makeRelative(phi);
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adjustPhi(phi, U, p);
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// Non-orthogonal velocity potential corrector loop
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while (potentialFlow.correctNonOrthogonal())
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{
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fvScalarMatrix PhiEqn
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(
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fvm::laplacian(dimensionedScalar("1", dimless, 1), Phi)
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==
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fvc::div(phi)
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);
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PhiEqn.setReference(PhiRefCell, PhiRefValue);
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PhiEqn.solve();
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if (potentialFlow.finalNonOrthogonalIter())
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{
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phi -= PhiEqn.flux();
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}
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}
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MRF.makeAbsolute(phi);
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Info<< "Continuity error = "
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<< mag(fvc::div(phi))().weightedAverage(mesh.V()).value()
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<< endl;
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U = fvc::reconstruct(phi);
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U.correctBoundaryConditions();
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Info<< "Interpolated velocity error = "
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<< (sqrt(sum(sqr((fvc::interpolate(U) & mesh.Sf()) - phi)))
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/sum(mesh.magSf())).value()
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<< endl;
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// Write U and phi
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U.write();
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phi.write();
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// Optionally write Phi
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if (args.optionFound("writePhi"))
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{
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Phi.write();
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}
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// Calculate the pressure field
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if (args.optionFound("writep"))
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{
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Info<< nl << "Calculating approximate pressure field" << endl;
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label pRefCell = 0;
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scalar pRefValue = 0.0;
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setRefCell
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(
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p,
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potentialFlow.dict(),
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pRefCell,
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pRefValue
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);
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// Calculate the flow-direction filter tensor
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volScalarField magSqrU(magSqr(U));
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volSymmTensorField F(sqr(U)/(magSqrU + SMALL*average(magSqrU)));
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// Calculate the divergence of the flow-direction filtered div(U*U)
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// Filtering with the flow-direction generates a more reasonable
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// pressure distribution in regions of high velocity gradient in the
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// direction of the flow
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volScalarField divDivUU
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(
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fvc::div
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(
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F & fvc::div(phi, U),
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"div(div(phi,U))"
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)
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);
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// Solve a Poisson equation for the approximate pressure
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while (potentialFlow.correctNonOrthogonal())
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{
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fvScalarMatrix pEqn
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(
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fvm::laplacian(p) + divDivUU
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);
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pEqn.setReference(pRefCell, pRefValue);
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pEqn.solve();
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}
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p.write();
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}
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runTime.functionObjects().end();
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Info<< "ExecutionTime = " << runTime.elapsedCpuTime() << " s"
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<< " ClockTime = " << runTime.elapsedClockTime() << " s"
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<< nl << endl;
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Info<< "End\n" << endl;
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return 0;
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}
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// ************************************************************************* //
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