
Classes | |
| class | sorptionWallFunctionFvPatchScalarField |
The sorptionWallFunction is a wall boundary condition to specify scalar/concentration gradient for turbulent and laminar flows. More... | |
| class | epsilonWallFunctionFvPatchScalarField |
This boundary condition provides wall functions for the turbulent kinetic energy dissipation rate (i.e. epsilon) and the turbulent kinetic energy production contribution (i.e. G) for low- and high-Reynolds number simulations. More... | |
| class | kLowReWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the turbulent kinetic energy (i.e. k) for low- and high-Reynolds number simulations. More... | |
| class | kqRWallFunctionFvPatchField< Type > |
This boundary condition provides a simple wrapper around the zero-gradient condition, which can be used for the turbulent kinetic energy (i.e. k), square-root of turbulent kinetic energy (i.e. q) and Reynolds stress symmetric-tensor fields (i.e. R) for the cases of high Reynolds number flow using wall functions. It is not a wall-function condition. More... | |
| class | nutkRoughWallFunctionFvPatchScalarField |
This boundary condition provides a wall-function for the turbulent viscosity (i.e. nut) when using wall functions for rough walls, based on the turbulent kinetic energy (i.e. k). The condition manipulates the wall roughness parameter (i.e. E) to account for roughness effects. More... | |
| class | nutkWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the turbulent viscosity (i.e. nut) based on the turbulent kinetic energy, (i.e. k) for for low- and high-Reynolds number applications. More... | |
| class | nutLowReWallFunctionFvPatchScalarField |
This boundary condition provides a simple wrapper around a zero fixed-value condition for the turbulent viscosity (i.e. nut) for low-Reynolds number applications. It sets nut to zero, and provides an access function to calculate y+. More... | |
| class | nutUBlendedWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the turbulent viscosity (i.e. nut) based on velocity (i.e. U) using a binomial-function wall-function blending method between the viscous and inertial sublayer predictions of nut for low- and high-Reynolds number applications. More... | |
| class | nutURoughWallFunctionFvPatchScalarField |
This boundary condition provides a wall function on the turbulent viscosity (i.e. nut) based on velocity (i.e. U) for low- and high-Reynolds number applications for rough walls. More... | |
| class | nutUSpaldingWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the turbulent viscosity (i.e. nut) based on velocity (i.e. U). Using Spalding's law gives a continuous nut profile to the wall. More... | |
| class | nutUTabulatedWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on the turbulent viscosity (i.e. nut) based on velocity (i.e. U), for low- and high-Reynolds number applications. More... | |
| class | nutUWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the turbulent viscosity (i.e. nut) based on velocity (i.e. U) for low- and high-Reynolds number applications. More... | |
| class | nutWallFunctionFvPatchScalarField |
The class nutWallFunction is an abstract base class that hosts ![]() nut wall-function boundary conditions. More... | |
| class | omegaWallFunctionFvPatchScalarField |
This boundary condition provides a wall function for the specific dissipation rate (i.e. omega) and the turbulent kinetic energy production contribution (i.e. G) for low- and high-Reynolds number applications. More... | |
This group contains turbulence model wall functions