Classes | |
| class | epsilonWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on 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 turbulence models. More... | |
| class | kLowReWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on the turbulent kinetic energy, i.e. k, for low- and high-Reynolds number turbulence models. 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 tensor fields, i.e. R, for the cases of high Reynolds number flow using wall functions. More... | |
| class | nutkRoughWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on 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 constraint on the turbulent viscosity, i.e. nut, based on the turbulent kinetic energy, i.e. k, for for low- and high-Reynolds number turbulence models. More... | |
| class | nutLowReWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on the turbulent viscosity, i.e. nut, for low Reynolds number models. It sets nut to zero, and provides an access function to calculate y+. More... | |
| class | nutUBlendedWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on 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 turbulence models. More... | |
| class | nutURoughWallFunctionFvPatchScalarField |
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 turbulence models for rough walls. More... | |
| class | nutUSpaldingWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on 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 turbulence models. More... | |
| class | nutUWallFunctionFvPatchScalarField |
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 turbulence models. More... | |
| class | nutWallFunctionFvPatchScalarField |
The class nutWallFunction is a base class that parents the derived boundary conditions which provide a wall constraint on various fields, such as turbulent viscosity, i.e. nut, or turbulent kinetic energy dissipation rate, i.e. epsilon, for low- and high-Reynolds number turbulence models. The class is not an executable itself, yet a provider for common entries to its derived boundary conditions. More... | |
| class | omegaWallFunctionFvPatchScalarField |
This boundary condition provides a wall constraint on the specific dissipation rate, i.e. omega, and the turbulent kinetic energy production contribution, i.e. G, for low- and high-Reynolds number turbulence models. More... | |
This group contains turbulence model wall functions