mirror of
https://develop.openfoam.com/Development/openfoam.git
synced 2025-11-28 03:28:01 +00:00
Adding overPotentialFoam and overRhoSimpleFoam and tutorials
This commit is contained in:
@ -0,0 +1,3 @@
|
||||
potentialFoam.C
|
||||
|
||||
EXE = $(FOAM_APPBIN)/overPotentialFoam
|
||||
@ -0,0 +1,12 @@
|
||||
EXE_INC = \
|
||||
-I$(LIB_SRC)/finiteVolume/lnInclude \
|
||||
-I$(LIB_SRC)/dynamicFvMesh/lnInclude \
|
||||
-I$(LIB_SRC)/overset/lnInclude \
|
||||
-I$(LIB_SRC)/meshTools/lnInclude \
|
||||
-I$(LIB_SRC)/sampling/lnInclude
|
||||
|
||||
EXE_LIBS = \
|
||||
-lfiniteVolume \
|
||||
-lmeshTools \
|
||||
-lsampling \
|
||||
-loverset
|
||||
@ -0,0 +1,9 @@
|
||||
const dictionary& potentialFlow
|
||||
(
|
||||
mesh.solutionDict().subDict("potentialFlow")
|
||||
);
|
||||
|
||||
const int nNonOrthCorr
|
||||
(
|
||||
potentialFlow.lookupOrDefault<int>("nNonOrthogonalCorrectors", 0)
|
||||
);
|
||||
@ -0,0 +1,146 @@
|
||||
Info<< "Reading velocity field U\n" << endl;
|
||||
volVectorField U
|
||||
(
|
||||
IOobject
|
||||
(
|
||||
"U",
|
||||
runTime.timeName(),
|
||||
mesh,
|
||||
IOobject::MUST_READ,
|
||||
IOobject::AUTO_WRITE
|
||||
),
|
||||
mesh
|
||||
);
|
||||
|
||||
// Initialise the velocity internal field to zero
|
||||
U = dimensionedVector("0", U.dimensions(), Zero);
|
||||
|
||||
surfaceScalarField phi
|
||||
(
|
||||
IOobject
|
||||
(
|
||||
"phi",
|
||||
runTime.timeName(),
|
||||
mesh,
|
||||
IOobject::NO_READ,
|
||||
IOobject::AUTO_WRITE
|
||||
),
|
||||
fvc::flux(U)
|
||||
);
|
||||
|
||||
if (args.optionFound("initialiseUBCs"))
|
||||
{
|
||||
U.correctBoundaryConditions();
|
||||
phi = fvc::flux(U);
|
||||
}
|
||||
|
||||
|
||||
// Construct a pressure field
|
||||
// If it is available read it otherwise construct from the velocity BCs
|
||||
// converting fixed-value BCs to zero-gradient and vice versa.
|
||||
word pName("p");
|
||||
|
||||
// Update name of the pressure field from the command-line option
|
||||
args.optionReadIfPresent("pName", pName);
|
||||
|
||||
// Infer the pressure BCs from the velocity
|
||||
wordList pBCTypes
|
||||
(
|
||||
U.boundaryField().size(),
|
||||
fixedValueFvPatchScalarField::typeName
|
||||
);
|
||||
|
||||
forAll(U.boundaryField(), patchi)
|
||||
{
|
||||
if (U.boundaryField()[patchi].fixesValue())
|
||||
{
|
||||
pBCTypes[patchi] = zeroGradientFvPatchScalarField::typeName;
|
||||
}
|
||||
}
|
||||
|
||||
// Note that registerObject is false for the pressure field. The pressure
|
||||
// field in this solver doesn't have a physical value during the solution.
|
||||
// It shouldn't be looked up and used by sub models or boundary conditions.
|
||||
Info<< "Constructing pressure field " << pName << nl << endl;
|
||||
volScalarField p
|
||||
(
|
||||
IOobject
|
||||
(
|
||||
pName,
|
||||
runTime.timeName(),
|
||||
mesh,
|
||||
IOobject::READ_IF_PRESENT,
|
||||
IOobject::NO_WRITE,
|
||||
false
|
||||
),
|
||||
mesh,
|
||||
dimensionedScalar(pName, sqr(dimVelocity), 0),
|
||||
pBCTypes
|
||||
);
|
||||
|
||||
// Infer the velocity potential BCs from the pressure
|
||||
wordList PhiBCTypes
|
||||
(
|
||||
p.boundaryField().size(),
|
||||
zeroGradientFvPatchScalarField::typeName
|
||||
);
|
||||
|
||||
forAll(p.boundaryField(), patchi)
|
||||
{
|
||||
if (p.boundaryField()[patchi].fixesValue())
|
||||
{
|
||||
PhiBCTypes[patchi] = fixedValueFvPatchScalarField::typeName;
|
||||
}
|
||||
}
|
||||
|
||||
Info<< "Constructing velocity potential field Phi\n" << endl;
|
||||
volScalarField Phi
|
||||
(
|
||||
IOobject
|
||||
(
|
||||
"Phi",
|
||||
runTime.timeName(),
|
||||
mesh,
|
||||
IOobject::READ_IF_PRESENT,
|
||||
IOobject::NO_WRITE
|
||||
),
|
||||
mesh,
|
||||
dimensionedScalar("Phi", dimLength*dimVelocity, 0),
|
||||
PhiBCTypes
|
||||
);
|
||||
|
||||
label PhiRefCell = 0;
|
||||
scalar PhiRefValue = 0;
|
||||
setRefCell
|
||||
(
|
||||
Phi,
|
||||
potentialFlow.dict(),
|
||||
PhiRefCell,
|
||||
PhiRefValue
|
||||
);
|
||||
mesh.setFluxRequired(Phi.name());
|
||||
|
||||
#include "createMRF.H"
|
||||
|
||||
// Add overset specific interpolations
|
||||
{
|
||||
dictionary oversetDict;
|
||||
oversetDict.add("Phi", true);
|
||||
oversetDict.add("U", true);
|
||||
|
||||
const_cast<dictionary&>
|
||||
(
|
||||
mesh.schemesDict()
|
||||
).add
|
||||
(
|
||||
"oversetInterpolationRequired",
|
||||
oversetDict,
|
||||
true
|
||||
);
|
||||
}
|
||||
|
||||
// Mask field for zeroing out contributions on hole cells
|
||||
#include "createCellMask.H"
|
||||
|
||||
// Create bool field with interpolated cells
|
||||
#include "createInterpolatedCells.H"
|
||||
@ -0,0 +1,260 @@
|
||||
/*---------------------------------------------------------------------------*\
|
||||
========= |
|
||||
\\ / F ield | OpenFOAM: The Open Source CFD Toolbox
|
||||
\\ / O peration |
|
||||
\\ / A nd | Copyright (C) 2017 OpenCFD Ltd
|
||||
\\/ M anipulation |
|
||||
-------------------------------------------------------------------------------
|
||||
License
|
||||
This file is part of OpenFOAM.
|
||||
|
||||
OpenFOAM 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.
|
||||
|
||||
OpenFOAM 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 OpenFOAM. If not, see <http://www.gnu.org/licenses/>.
|
||||
|
||||
Application
|
||||
potentialFoam
|
||||
|
||||
Group
|
||||
grpBasicSolvers
|
||||
|
||||
Description
|
||||
Potential flow solver which solves for the velocity potential, to
|
||||
calculate the flux-field, from which the velocity field is obtained by
|
||||
reconstructing the flux.
|
||||
|
||||
\heading Solver details
|
||||
The potential flow solution is typically employed to generate initial fields
|
||||
for full Navier-Stokes codes. The flow is evolved using the equation:
|
||||
|
||||
\f[
|
||||
\laplacian \Phi = \div(\vec{U})
|
||||
\f]
|
||||
|
||||
Where:
|
||||
\vartable
|
||||
\Phi | Velocity potential [m2/s]
|
||||
\vec{U} | Velocity [m/s]
|
||||
\endvartable
|
||||
|
||||
The corresponding pressure field could be calculated from the divergence
|
||||
of the Euler equation:
|
||||
|
||||
\f[
|
||||
\laplacian p + \div(\div(\vec{U}\otimes\vec{U})) = 0
|
||||
\f]
|
||||
|
||||
but this generates excessive pressure variation in regions of large
|
||||
velocity gradient normal to the flow direction. A better option is to
|
||||
calculate the pressure field corresponding to velocity variation along the
|
||||
stream-lines:
|
||||
|
||||
\f[
|
||||
\laplacian p + \div(\vec{F}\cdot\div(\vec{U}\otimes\vec{U})) = 0
|
||||
\f]
|
||||
where the flow direction tensor \f$\vec{F}\f$ is obtained from
|
||||
\f[
|
||||
\vec{F} = \hat{\vec{U}}\otimes\hat{\vec{U}}
|
||||
\f]
|
||||
|
||||
\heading Required fields
|
||||
\plaintable
|
||||
U | Velocity [m/s]
|
||||
\endplaintable
|
||||
|
||||
\heading Optional fields
|
||||
\plaintable
|
||||
p | Kinematic pressure [m2/s2]
|
||||
Phi | Velocity potential [m2/s]
|
||||
| Generated from p (if present) or U if not present
|
||||
\endplaintable
|
||||
|
||||
\heading Options
|
||||
\plaintable
|
||||
-writep | write the Euler pressure
|
||||
-writePhi | Write the final velocity potential
|
||||
-initialiseUBCs | Update the velocity boundaries before solving for Phi
|
||||
\endplaintable
|
||||
|
||||
\*---------------------------------------------------------------------------*/
|
||||
|
||||
#include "fvCFD.H"
|
||||
#include "pisoControl.H"
|
||||
#include "dynamicFvMesh.H"
|
||||
#include "cellCellStencilObject.H"
|
||||
#include "localMin.H"
|
||||
|
||||
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
|
||||
|
||||
int main(int argc, char *argv[])
|
||||
{
|
||||
argList::addOption
|
||||
(
|
||||
"pName",
|
||||
"pName",
|
||||
"Name of the pressure field"
|
||||
);
|
||||
|
||||
argList::addBoolOption
|
||||
(
|
||||
"initialiseUBCs",
|
||||
"Initialise U boundary conditions"
|
||||
);
|
||||
|
||||
argList::addBoolOption
|
||||
(
|
||||
"writePhi",
|
||||
"Write the final velocity potential field"
|
||||
);
|
||||
|
||||
argList::addBoolOption
|
||||
(
|
||||
"writep",
|
||||
"Calculate and write the Euler pressure field"
|
||||
);
|
||||
|
||||
argList::addBoolOption
|
||||
(
|
||||
"withFunctionObjects",
|
||||
"execute functionObjects"
|
||||
);
|
||||
|
||||
#include "setRootCase.H"
|
||||
#include "createTime.H"
|
||||
#include "createNamedDynamicFvMesh.H"
|
||||
|
||||
pisoControl potentialFlow(mesh, "potentialFlow");
|
||||
|
||||
#include "createFields.H"
|
||||
|
||||
// * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * //
|
||||
|
||||
Info<< nl << "Calculating potential flow" << endl;
|
||||
|
||||
mesh.update();
|
||||
|
||||
surfaceScalarField faceMask(localMin<scalar>(mesh).interpolate(cellMask));
|
||||
|
||||
// Since solver contains no time loop it would never execute
|
||||
// function objects so do it ourselves
|
||||
runTime.functionObjects().start();
|
||||
|
||||
MRF.makeRelative(phi);
|
||||
adjustPhi(phi, U, p);
|
||||
|
||||
// Non-orthogonal velocity potential corrector loop
|
||||
while (potentialFlow.correct())
|
||||
{
|
||||
phi = fvc::flux(U);
|
||||
|
||||
while (potentialFlow.correctNonOrthogonal())
|
||||
{
|
||||
fvScalarMatrix PhiEqn
|
||||
(
|
||||
fvm::laplacian(faceMask, Phi)
|
||||
==
|
||||
fvc::div(phi)
|
||||
);
|
||||
|
||||
PhiEqn.setReference(PhiRefCell, PhiRefValue);
|
||||
PhiEqn.solve();
|
||||
|
||||
if (potentialFlow.finalNonOrthogonalIter())
|
||||
{
|
||||
phi -= PhiEqn.flux();
|
||||
}
|
||||
}
|
||||
|
||||
MRF.makeAbsolute(phi);
|
||||
|
||||
Info<< "Continuity error = "
|
||||
<< mag(fvc::div(phi))().weightedAverage(mesh.V()).value()
|
||||
<< endl;
|
||||
|
||||
U = fvc::reconstruct(phi);
|
||||
U.correctBoundaryConditions();
|
||||
|
||||
Info<< "Interpolated velocity error = "
|
||||
<< (sqrt(sum(sqr(fvc::flux(U) - phi)))/sum(mesh.magSf())).value()
|
||||
<< endl;
|
||||
}
|
||||
|
||||
// Write U and phi
|
||||
U.write();
|
||||
phi.write();
|
||||
|
||||
// Optionally write Phi
|
||||
if (args.optionFound("writePhi"))
|
||||
{
|
||||
Phi.write();
|
||||
}
|
||||
|
||||
// Calculate the pressure field from the Euler equation
|
||||
if (args.optionFound("writep"))
|
||||
{
|
||||
Info<< nl << "Calculating approximate pressure field" << endl;
|
||||
|
||||
label pRefCell = 0;
|
||||
scalar pRefValue = 0.0;
|
||||
setRefCell
|
||||
(
|
||||
p,
|
||||
potentialFlow.dict(),
|
||||
pRefCell,
|
||||
pRefValue
|
||||
);
|
||||
|
||||
// Calculate the flow-direction filter tensor
|
||||
volScalarField magSqrU(magSqr(U));
|
||||
volSymmTensorField F(sqr(U)/(magSqrU + SMALL*average(magSqrU)));
|
||||
|
||||
// Calculate the divergence of the flow-direction filtered div(U*U)
|
||||
// Filtering with the flow-direction generates a more reasonable
|
||||
// pressure distribution in regions of high velocity gradient in the
|
||||
// direction of the flow
|
||||
volScalarField divDivUU
|
||||
(
|
||||
fvc::div
|
||||
(
|
||||
F & fvc::div(phi, U),
|
||||
"div(div(phi,U))"
|
||||
)
|
||||
);
|
||||
|
||||
// Solve a Poisson equation for the approximate pressure
|
||||
while (potentialFlow.correctNonOrthogonal())
|
||||
{
|
||||
fvScalarMatrix pEqn
|
||||
(
|
||||
fvm::laplacian(p) + divDivUU
|
||||
);
|
||||
|
||||
pEqn.setReference(pRefCell, pRefValue);
|
||||
pEqn.solve();
|
||||
}
|
||||
|
||||
p.write();
|
||||
}
|
||||
|
||||
runTime.functionObjects().end();
|
||||
|
||||
Info<< "ExecutionTime = " << runTime.elapsedCpuTime() << " s"
|
||||
<< " ClockTime = " << runTime.elapsedClockTime() << " s"
|
||||
<< nl << endl;
|
||||
|
||||
Info<< "End\n" << endl;
|
||||
|
||||
return 0;
|
||||
}
|
||||
|
||||
|
||||
// ************************************************************************* //
|
||||
Reference in New Issue
Block a user