Use the Thermophoretic Force node to exert the thermophoretic force on particles. The phenomenon called thermophoresis causes particles to migrate in a fluid with a nonuniform temperature field.
The model inputs for the Temperature T (SI unit: K) and
Absolute pressure pA (SI unit: Pa) are always shown in the settings window for this feature, even if there are no material properties that depend on them.
If the Include rarefaction effects check box is selected in the physics interface
Particle Release and Propagation section, select an option from the
Thermophoretic force model list. Some of these options are only applicable for certain Knudsen number ranges:
When the Include rarefaction effects check box is cleared, the fluid is always treated as a continuum (low Knudsen number) flow, and only the Epstein model is used.
The following fluid parameters all take default values From material or can be computed from another physics interface. Or select
User defined to enter a value or expression for the:
If the Waldmann,
Talbot, or
Linearized BGK model is used, also enter the
Background gas molar mass Mg (SI unit: kg/mol). The default is
0.04 kg/mol.
If the Waldmann,
Talbot, or
Linearized BGK model is used, select an option from the
Mean free path calculation list:
Ideal gas, hard sphere collisions or
User-defined correction. For
User-defined correction enter a
Mean free path correction λ'/
λ by which the mean free path differs from the value for hard spheres in an ideal gas.
If the Linearized BGK model is used, enter an
Energy accommodation coefficient αE (dimensionless) and a
Momentum accommodation coefficient αM (dimensionless). The default values are
1.
Enter a value or expression for the Thermophoretic correction factor Cs (dimensionless). The default is
1.17. If the
Talbot model is used, enter two additional dimensionless thermophoretic correction factors
Cm and
Ct. The default values are
1.146 and
2.2, respectively.
Select the Use piecewise polynomial recovery on field check box to smooth the temperature using piecewise polynomial recovery. This can give a much more accurate representation of the temperature as it uses information on adjacent mesh elements to reconstruct the field. If a coarse mesh is used to compute the field then this option can be especially useful.
Use the Particles to affect list to apply the force to specific particles. The available settings are the same as for the
Force node.