forceModel GidaspowDrag command¶
Syntax¶
Defined in couplingProperties dictionary.
forceModels
(
GidaspowDrag
);
GidaspowDragProps
{
velFieldName "U";
voidfractionFieldName "voidfraction";
granVelFieldName "Us";
phi scalar1;
scale scalar2;
scaleDrag scalar3;
switchingVoidfraction scalar4;
treatForceExplicit switch1;
implForceDEM switch2;
verbose switch3;
interpolation switch4;
scalarViscosity switch5;
}
U = name of the finite volume fluid velocity field
voidfraction = name of the finite volume void fraction field
Us = name of the finite volume cell averaged particle velocity field
scalar1 = drag correction factor (in doubt 1)
scalar2 = (optional, default 1.0) scaling of particle diameter: d_sim=scale*d_real. d_sim=(potentially coarse-grained) particle diameter. scale=coarse-graining factor. d_real= particle diameter as it is measured.
scalar3 = (optional, default 1.0) scaling of drag law
scalar4 = (optional, default 0.8) void fraction above which dilute formulation will be used
switch1 = (optional, default false) sub model switch, see forceSubModel for details
switch2 = (optional, default false) flag to use implicit formulation of drag on DEM side
switch3 = (optional, default false) sub model switch, see forceSubModel for details
switch4 = (optional, default false) flag to use interpolated void fraction and fluid velocity values
switch5 = (optional, default false) sub model switch, see forceSubModel for details
Examples¶
forceModels
(
GidaspowDrag
);
GidaspowDragProps
{
velFieldName "U";
voidfractionFieldName "voidfraction";
granVelFieldName "Us";
}
Description¶
The force model performs the calculation of forces (e.g. fluid-particle interaction forces) acting on each DEM particle. The GidaspowDrag model is a model that calculates the particle based drag force following the correlation of Gidaspow which is a combination of Ergun (1952) and Wen & Yu (1966) (see Zhu et al. (2007): “Discrete particle simulation of particulate systems: Theoretical developments”, ChemEngScience).
Restrictions¶
none