Difference between revisions of "ChtMultiRegionFoam"
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====Energy conservation==== | ====Energy conservation==== | ||
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+ | The energy equation can be found in: https://cfd.direct/openfoam/energy-equation/ | ||
===Equations Solid=== | ===Equations Solid=== | ||
==Source Code== | ==Source Code== |
Revision as of 19:48, 2 November 2018
ChtMultiRegionFoam
Solver for steady or transient fluid flow and solid heat conduction, with conjugate heat transfer between regions, buoyancy effects, turbulence, reactions and radiation modelling.
Contents
1 Equations
For each region defined as fluid, the according equation for the fluid is solved and the same is done for each solid region. The regions are coupled by a thermal boundary condition.
1.1 Equations Fluid
For each fluid region the compressible Navier Stokes equation are solved.
1.1.1 Mass conservation
The variable-density continuity equation is
| (1) |
The source code can be found in src/finiteVolume/cfdTools/compressible/rhoEqn.H:
{ fvScalarMatrix rhoEqn ( fvm::ddt(rho) + fvc::div(phi) == fvOptions(rho) ); fvOptions.constrain(rhoEqn); rhoEqn.solve(); fvOptions.correct(rho); }
1.1.2 Momentum conservation
| (2) |
represent the velocity, the gravitational acceleration, the pressure minus the hydrostatic pressure and and are the viscose and turbulent stresses.
The source code can be found in Ueqn.H:
// Solve the Momentum equation MRF.correctBoundaryVelocity(U); tmp<fvVectorMatrix> tUEqn ( fvm::ddt(rho, U) + fvm::div(phi, U) + MRF.DDt(rho, U) + turbulence.divDevRhoReff(U) == fvOptions(rho, U) ); fvVectorMatrix& UEqn = tUEqn.ref(); UEqn.relax(); fvOptions.constrain(UEqn); if (pimple.momentumPredictor()) { solve ( UEqn == fvc::reconstruct ( ( - ghf*fvc::snGrad(rho) - fvc::snGrad(p_rgh) )*mesh.magSf() ) ); fvOptions.correct(U); K = 0.5*magSqr(U); } fvOptions.correct(U);
1.1.3 Energy conservation
The energy equation can be found in: https://cfd.direct/openfoam/energy-equation/