diff --git a/applications/solvers/cfdemSolverRhoPimple/cfdemSolverRhoPimpleChem/EEqn.H b/applications/solvers/cfdemSolverRhoPimple/cfdemSolverRhoPimpleChem/EEqn.H deleted file mode 100644 index ae52bae5..00000000 --- a/applications/solvers/cfdemSolverRhoPimple/cfdemSolverRhoPimpleChem/EEqn.H +++ /dev/null @@ -1,44 +0,0 @@ -// contributions to internal energy equation can be found in -// Crowe et al.: "Multiphase flows with droplets and particles", CRC Press 1998 - -{ - // dim he = J / kg - volScalarField& he = thermo.he(); - particleCloud.energyContributions(Qsource); - - - fvScalarMatrix EEqn - ( - fvm::ddt(rhoeps, he) + fvm::div(phi, he) - + fvc::ddt(rhoeps, K) + fvc::div(phi, K) - + ( - he.name() == "e" - ? fvc::div - ( - fvc::absolute(phi/fvc::interpolate(rho), voidfraction*U), - p, - "div(phiv,p)" - ) - : -dpdt - ) - // net heat transfer from particles to fluid - - Qsource - // thermal conduction of the fluid with effective conductivity - - fvc::laplacian(rhoeps*particleCloud.thermCondM().thermDiff(),he) - - // + particle-fluid energy transfer due to work - // + fluid energy dissipation due to shearing - == - fvOptions(rho, he) - ); - - EEqn.relax(); - - fvOptions.constrain(EEqn); - - EEqn.solve(); - - fvOptions.correct(he); - - thermo.correct(); -} diff --git a/tutorials/cfdemSolverRhoPimpleChem/simplifiedSiwek_in_CFDEM/CFD/constant/transportProperties b/tutorials/cfdemSolverRhoPimpleChem/simplifiedSiwek_in_CFDEM/CFD/constant/transportProperties index 63cdca8c..47c0b1a4 100644 --- a/tutorials/cfdemSolverRhoPimpleChem/simplifiedSiwek_in_CFDEM/CFD/constant/transportProperties +++ b/tutorials/cfdemSolverRhoPimpleChem/simplifiedSiwek_in_CFDEM/CFD/constant/transportProperties @@ -19,6 +19,10 @@ transportModel Newtonian; nu nu [ 0 2 -1 0 0 0 0 ] 1.5e-04; +kf kf [ 1 1 -3 -1 0 0 0 ] 0; + +Cp Cp [ 0 2 -2 -1 0 0 0 ] 1; + CrossPowerLawCoeffs { nu0 nu0 [ 0 2 -1 0 0 0 0 ] 1e-06; @@ -35,6 +39,4 @@ BirdCarreauCoeffs n n [ 0 0 0 0 0 0 0 ] 1; } -kf kf [ 0 0 0 0 0 0 0 ] 0; -Cp Cp [ 0 0 0 0 0 0 0 ] 0; // ************************************************************************* //