The Wilcox R-ω Turbulence Model
The Wilcox R-ω model belongs to RANS-RSM type of turbulence models and, hence, does not assume a particular form of (the kinematic Reynolds stress tensor). It solves the transport equation for R instead, complemented by the transport equation for the turbulence specific dissipation rate ω, which allows to capture the evolution of turbulence structure properly Ref. 32. This leads to more accurate prediction of separation, transient phenomena, effects of swirl and curvature. Moreover, correct description of secondary flows is achieved, which eddy-viscosity based models are intrinsically incapable of.
In COMSOL Multiphysics the equations for the Wilcox R-ω model are implemented in fully compressible form and are compatible with most Multiphysics Couplings available for a RANS-EVM.
The set of Wilcox R-ω model parameters with their default values is
(3-186)
The expressions for the turbulence kinetic energy, turbulence viscosity, turbulence dissipation rate, turbulence time-scale, and turbulence frequency-scale are
(3-187)
The turbulence anisotropy tensor is defined as
(3-188)
The R-equation is stated as
(3-189)
This is a symmetric tensor equation that consists of six scalar equations. The production term Pij (as well as P - production term of k) has explicit form
(3-190)
Of primary importance for a Reynolds Stress Model is the modeling of the pressure–strain correlation Πij:
(3-191)
which is responsible for the redistribution of the turbulence kinetic energy among the components of R. For Wilcox R-ω it involves two model parameters.
The turbulent diffusion D and turbulent dissipation εij of R are modeled as
(3-192)
The ω-equation is stated as
(3-193)
where
(3-194)
Wall Distance
The wall distance variable, lw, is provided by a mathematical Wall Distance interface that is included when using the Wilcox R-ω model. The solution to the wall distance equation is controlled using the parameter lref. The distance to objects larger than lref is represented accurately, while objects smaller than lref are effectively diminished by appearing to be farther away than they actually are. This is a desirable feature in turbulence modeling since small objects would get too large an impact on the solution if the wall distance were measured exactly.
When there is no Moving Mesh, the equation for the wall distance variable can be solved once only. A Wall Distance Initialization study type is provided for this purpose and should be added before the actual Stationary or Time Dependent study step.
Wall Boundary Conditions
Low Reynolds Number Wall Treatment
The Wilcox R-ω turbulence model can be integrated all the way down to the wall and is consistent with the no-slip condition u = 0. Since fluctuations of velocity must disappear on the wall, so must R. Hence, R = 0 on the wall.
The corresponding boundary condition for ω is
(3-195)
To avoid the singularity at the wall, ω is not solved for in the cells adjacent to a solid wall. Instead, its value is prescribed by Equation 3-195 (using the variable ωw, which only exists in those cells). Accurate solutions in the near-wall region require that the wall resolution in viscous units
(3-196)
where the resolution height is based on the distance between the first computational node inside the domain and the wall. uτ is the friction velocity which is calculated from the wall shear-stress τw,
(3-197)
and is available as the postprocessing variable (u_tauWall). Also, the boundary variable Distance to cell center in viscous units, (lplus_cc), is available to ensure that the mesh is fine enough. is the distance, measured in viscous units, from the wall to the center of the wall adjacent cell, thus and according to Equation 3-196 should be about 0.5. Observe that very small values of can reduce the convergence rate. Also notice that it is unlikely that a solution is obtained at all if
Since the ωw variable requires the wall distance, a wall distance equation must be solved prior to solving the Wilcox R-ω model.
The postprocessing variable Wall resolution in viscous units, (Delta_wPlus), is available.
Inlet Values for the Turbulence Length Scale and Intensity
The guidelines given in Inlet Values for the Turbulence Length Scale and Turbulent Intensity for selecting the turbulence length scale, LT, and the turbulence intensity, IT, apply also to the Wilcox R-ω model.
Initial Values
The Wilcox R-ω model essentially has the same default initial guess as the SST model, but for the Reynolds stress tensor instead of k:
The default initial value for the wall distance equation (which solves for the reciprocal wall distance) is 2/lref.
Scaling for Time-Dependent Simulations
The Wilcox R-ω model applies absolute scales of the same type as the SST model, namely
In the COMSOL Multiphysics Reference Manual: