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foam-extend4.1-coherent-io/applications/solvers/electromagnetics/mhdFoam/mhdFoam.C
2016-06-21 15:04:12 +02:00

168 lines
4.9 KiB
C

/*---------------------------------------------------------------------------*\
========= |
\\ / F ield | foam-extend: Open Source CFD
\\ / O peration | Version: 4.0
\\ / A nd | Web: http://www.foam-extend.org
\\/ M anipulation | For copyright notice see file Copyright
-------------------------------------------------------------------------------
License
This file is part of foam-extend.
foam-extend is free software: you can redistribute it and/or modify it
under the terms of the GNU General Public License as published by the
Free Software Foundation, either version 3 of the License, or (at your
option) any later version.
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.
You should have received a copy of the GNU General Public License
along with foam-extend. If not, see <http://www.gnu.org/licenses/>.
Application
mhdFoam
Description
Solver for magnetohydrodynamics (MHD): incompressible, laminar flow of a
conducting fluid under the influence of a magnetic field.
An applied magnetic field H acts as a driving force,
at present boundary conditions cannot be set via the
electric field E or current density J. The fluid viscosity nu,
conductivity sigma and permeability mu are read in as uniform
constants.
A fictitous magnetic flux pressure pH is introduced in order to
compensate for discretisation errors and create a magnetic face flux
field which is divergence free as required by Maxwell's equations.
However, in this formulation discretisation error prevents the normal
stresses in UB from cancelling with those from BU, but it is unknown
whether this is a serious error. A correction could be introduced
whereby the normal stresses in the discretised BU term are replaced
by those from the UB term, but this would violate the boundedness
constraint presently observed in the present numerics which
guarantees div(U) and div(H) are zero.
\*---------------------------------------------------------------------------*/
#include "fvCFD.H"
#include "OSspecific.H"
#include "pisoControl.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
int main(int argc, char *argv[])
{
# include "setRootCase.H"
# include "createTime.H"
# include "createMesh.H"
pisoControl piso(mesh);
# include "createFields.H"
# include "initContinuityErrs.H"
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
Info<< nl << "Starting time loop" << endl;
while (runTime.loop())
{
# include "readBPISOControls.H"
Info<< "Time = " << runTime.timeName() << nl << endl;
# include "CourantNo.H"
{
fvVectorMatrix UEqn
(
fvm::ddt(U)
+ fvm::div(phi, U)
- fvc::div(phiB, 2.0*DBU*B)
- fvm::laplacian(nu, U)
+ fvc::grad(DBU*magSqr(B))
);
solve(UEqn == -fvc::grad(p));
// --- PISO loop
while (piso.correct())
{
volScalarField rUA = 1.0/UEqn.A();
U = rUA*UEqn.H();
phi = (fvc::interpolate(U) & mesh.Sf())
+ fvc::ddtPhiCorr(rUA, U, phi);
while (piso.correctNonOrthogonal())
{
fvScalarMatrix pEqn
(
fvm::laplacian(rUA, p) == fvc::div(phi)
);
pEqn.setReference(pRefCell, pRefValue);
pEqn.solve();
if (piso.finalNonOrthogonalIter())
{
phi -= pEqn.flux();
}
}
# include "continuityErrs.H"
U -= rUA*fvc::grad(p);
U.correctBoundaryConditions();
}
}
// --- B-PISO loop
for (int Bcorr=0; Bcorr<nBcorr; Bcorr++)
{
fvVectorMatrix BEqn
(
fvm::ddt(B)
+ fvm::div(phi, B)
- fvc::div(phiB, U)
- fvm::laplacian(DB, B)
);
BEqn.solve();
volScalarField rBA = 1.0/BEqn.A();
phiB = (fvc::interpolate(B) & mesh.Sf())
+ fvc::ddtPhiCorr(rBA, B, phiB);
fvScalarMatrix pBEqn
(
fvm::laplacian(rBA, pB) == fvc::div(phiB)
);
pBEqn.solve();
phiB -= pBEqn.flux();
# include "magneticFieldErr.H"
}
runTime.write();
}
Info<< "End\n" << endl;
return 0;
}
// ************************************************************************* //