forceModel LaEuScalarTemp command¶
Syntax¶
Defined in couplingProperties dictionary.
forceModels
(
LaEuScalarTemp
);
LaEuScalarTempProps
{
velFieldName "U";
tempFieldName "T";
voidfractionFieldName "voidfraction";
partTempName "Temp";
partHeatFluxName "convectiveHeatFlux";
lambda scalar1;
Cp scalar2;
maxSource scalar3;
verbose switch1;
interpolation switch2;
scalarViscosity switch3;
}
U = name of the finite volume fluid velocity field
T = name of the finite volume scalar temperature field
voidfraction = name of the finite volume void fraction field
Temp = name of the DEM data representing the particles temperature
convectiveHeatFlux = name of the DEM data representing the particle-fluid convective heat flux
scalar1 = fluid thermal conductivity [W/(m*K)]
scalar2 = fluid specific heat capacity [W*s/(kg*K)]
scalar3 = (optional, default 1e30) limit maximal turbulence
switch1 = (optional, default false) for verbose run
switch2 = (optional, default false) flag to use interpolated void fraction and fluid velocity values
switch3 = (optional, default false) sub model switch, see forceSubModel for details
Examples¶
forceModels
(
LaEuScalarTemp
);
LaEuScalarTempProps
{
velFieldName "U";
tempFieldName "T";
voidfractionFieldName "voidfraction";
partTempName "Temp";
partHeatFluxName "convectiveHeatFlux";
lambda 0.0256;
Cp 1007;
}
Description¶
This “force model” does not influence the particles or the fluid flow! Using the particles’ temperature a scalar field representing “particle-fluid heat flux” is calculated. The solver then uses this source field in the scalar transport equation for the temperature. The model for convective heat transfer is based on Li and Mason (2000), A computational investigation of transient heat transfer in pneumatic transport of granular particles, Pow.Tech 112
Restrictions¶
Goes only with cfdemSolverPisoScalar. The force model has to be the second (!!!) model in the forces list.