incompressible/nonNewtonianIcoFoam, solver + tutorials
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2 changed files with 27 additions and 14 deletions
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@ -26,6 +26,10 @@ Application
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Description
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Transient solver for incompressible, laminar flow of non-Newtonian fluids.
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Consistent formulation without time-step and relaxation dependence by Jasak
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Author
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Hrvoje Jasak, Wikki Ltd. All rights reserved
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\*---------------------------------------------------------------------------*/
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@ -39,7 +43,7 @@ int main(int argc, char *argv[])
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# include "setRootCase.H"
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# include "createTime.H"
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# include "createMeshNoClear.H"
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# include "createMesh.H"
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# include "createFields.H"
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# include "initContinuityErrs.H"
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@ -56,24 +60,28 @@ int main(int argc, char *argv[])
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fluid.correct();
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fvVectorMatrix UEqn
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// Convection-diffusion matrix
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fvVectorMatrix HUEqn
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(
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fvm::ddt(U)
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+ fvm::div(phi, U)
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fvm::div(phi, U)
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- fvm::laplacian(fluid.nu(), U)
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);
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solve(UEqn == -fvc::grad(p));
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// Time derivative matrix
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fvVectorMatrix ddtUEqn(fvm::ddt(U));
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solve(ddtUEqn + HUEqn == -fvc::grad(p));
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// Prepare clean Ap without time derivative contribution
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// HJ, 26/Oct/2015
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volScalarField aU = HUEqn.A();
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// --- PISO loop
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for (int corr = 0; corr < nCorr; corr++)
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{
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volScalarField rUA = 1.0/UEqn.A();
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U = rUA*UEqn.H();
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phi = (fvc::interpolate(U) & mesh.Sf())
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+ fvc::ddtPhiCorr(rUA, U, phi);
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U = HUEqn.H()/aU;
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phi = (fvc::interpolate(U) & mesh.Sf());
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adjustPhi(phi, U, p);
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@ -81,7 +89,7 @@ int main(int argc, char *argv[])
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{
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fvScalarMatrix pEqn
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(
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fvm::laplacian(rUA, p) == fvc::div(phi)
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fvm::laplacian(1/aU, p) == fvc::div(phi)
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);
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pEqn.setReference(pRefCell, pRefValue);
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@ -95,7 +103,12 @@ int main(int argc, char *argv[])
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# include "continuityErrs.H"
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U -= rUA*fvc::grad(p);
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// Note: cannot call H(U) here because the velocity is not complete
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// HJ, 22/Jan/2016
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U = 1.0/(aU + ddtUEqn.A())*
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(
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U*aU - fvc::grad(p) + ddtUEqn.H()
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);
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U.correctBoundaryConditions();
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}
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@ -28,7 +28,7 @@ gradSchemes
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divSchemes
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{
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default none;
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div(phi,U) Gauss linear;
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div(phi,U) Gauss linearUpwind leastSquares;
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}
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laplacianSchemes
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