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