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foam-extend4.1-coherent-io/applications/solvers/solidMechanics/elasticPlasticNonLinULSolidFoam/elasticPlasticNonLinULSolidFoam.C

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/*---------------------------------------------------------------------------*\
========= |
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\\ / F ield | foam-extend: Open Source CFD
\\ / O peration | Version: 3.2
\\ / A nd | Web: http://www.foam-extend.org
\\/ M anipulation | For copyright notice see file Copyright
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-------------------------------------------------------------------------------
License
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This file is part of foam-extend.
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foam-extend 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 the
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Free Software Foundation, either version 3 of the License, or (at your
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option) any later version.
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foam-extend is distributed in the hope that it will be useful, but
WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
General Public License 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 foam-extend. If not, see <http://www.gnu.org/licenses/>.
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Application
elasticPlasticNonLinULSolidFoam
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Description
Finite volume structural solver employing a incremental strain updated
Lagrangian approach.
Valid for small strains, finite displacements and finite rotations.
Note: the reason the solver is not strictly valid for large strains is
because the constitutive stiffness tensor is not rotated.
For an updated Lagrangian solver which does rotate the stiffness tensor, and
hence is strictly Valid for large strains, use
elasticOrthoNonLinULSolidFoam.
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Author
Philip Cardiff UCD
Aitken relaxation by T. Tang DTU
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\*---------------------------------------------------------------------------*/
#include "fvCFD.H"
#include "constitutiveModel.H"
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#include "volPointInterpolation.H"
#include "pointPatchInterpolation.H"
#include "primitivePatchInterpolation.H"
#include "pointFields.H"
#include "twoDPointCorrector.H"
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#include "leastSquaresVolPointInterpolation.H"
#include "transformGeometricField.H"
#include "solidContactFvPatchVectorField.H"
#include "pointMesh.H"
#include "symmetryPolyPatch.H"
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// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
int main(int argc, char *argv[])
{
# include "setRootCase.H"
# include "createTime.H"
# include "createMesh.H"
# include "createFields.H"
# include "createHistory.H"
# include "readDivDSigmaExpMethod.H"
# include "readDivDSigmaNonLinExpMethod.H"
# include "readMoveMeshMethod.H"
# include "findGlobalFaceZones.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
Info<< "\nStarting time loop\n" << endl;
while(runTime.loop())
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{
Info<< "Time = " << runTime.timeName() << nl << endl;
# include "readSolidMechanicsControls.H"
int iCorr = 0;
lduMatrix::solverPerformance solverPerf;
scalar initialResidual = 0;
scalar relativeResidual = 1.0;
lduMatrix::debug = 0;
do
{
DU.storePrevIter();
# include "calculateDivDSigmaExp.H"
# include "calculateDivDSigmaNonLinExp.H"
// Updated lagrangian large strain momentum equation
fvVectorMatrix DUEqn
(
fvm::d2dt2(rho,DU)
==
fvm::laplacian(2*muf + lambdaf, DU, "laplacian(DDU,DU)")
+ divDSigmaExp
+ divDSigmaNonLinExp
//- fvc::div(2*mu*DEpsilonP, "div(sigma)")
- fvc::div(2*muf*( mesh.Sf() & fvc::interpolate(DEpsilonP)) )
);
if(nonLinearSemiImplicit)
{
// experimental
// we can treat the nonlinear term (gradDU & gradDU.T()) in a
// semi-implicit over-relaxed manner
// this should improve convergence when gradDU is large
// but maybe not execution time
DUEqn -=
fvm::laplacian
(
(2*mu + lambda)*gradDU, DU, "laplacian(DDU,DU)"
)
- fvc::div( (2*mu + lambda)*(gradDU&gradDU), "div(sigma)");
}
solverPerf = DUEqn.solve();
if(iCorr == 0)
{
initialResidual = solverPerf.initialResidual();
}
if(aitkenRelax)
{
# include "aitkenRelaxation.H"
}
else
{
DU.relax();
}
gradDU = fvc::grad(DU);
// correct plasticty term
rheology.correct();
// correct elastic properties
// for nonlinear elastic materials
//mu = rheology.newMu();
//lambda = rheology.newLambda();
//muf = fvc::interpolate(mu);
//lambdaf = fvc::interpolate(lambda);
# include "calculateDEpsilonDSigma.H"
# include "calculateRelativeResidual.H"
if(iCorr % infoFrequency == 0)
{
Info<< "\tTime " << runTime.value()
<< ", Corrector " << iCorr
<< ", Solving for " << DU.name()
<< " using " << solverPerf.solverName()
<< ", res = " << solverPerf.initialResidual()
<< ", rel res = " << relativeResidual;
if(aitkenRelax)
{
Info<< ", aitken = " << aitkenTheta;
}
Info<< ", iters = " << solverPerf.nIterations() << endl;
}
}
while
(
iCorr++ < 2
||
(
//solverPerf.initialResidual() > convergenceTolerance
relativeResidual > convergenceTolerance
&& iCorr < nCorr
)
);
Info<< nl << "Time " << runTime.value() << ", Solving for " << DU.name()
<< ", Initial residual = " << initialResidual
<< ", Final residual = " << solverPerf.initialResidual()
<< ", Final rel residual = " << relativeResidual
<< ", No outer iterations " << iCorr << endl;
rheology.updateYieldStress();
U += DU;
epsilon += DEpsilon;
epsilonP += DEpsilonP;
sigma += DSigma;
# include "moveMesh.H"
# include "rotateFields.H"
# include "writeFields.H"
# include "writeHistory.H"
Info<< nl << "ExecutionTime = " << runTime.elapsedCpuTime() << " s"
<< " ClockTime = " << runTime.elapsedClockTime() << " s"
<< endl;
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}
Info<< "End\n" << endl;
return(0);
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}
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// ************************************************************************* //