Modeling > Modeling Turbulence > Using Spalart-Allmaras Turbulence > What Are the Spalart-Allmaras Turbulence Models? > What Is the Spalart-Allmaras Detached Eddy Model?

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What Is the Spalart-Allmaras Detached Eddy Model?

Detached eddy simulation (DES) [27] is a modeling approach that combines features of Reynolds-Averaged (RANS) simulation in part of the flow and large eddy simulation (LES) in unsteady, separated regions. The DES version of the Spalart-Allmaras model contains modifications to the damping functions recommended by Squires et al. [29]. These modifications do not affect the predictions of fully turbulent flows, but prevent spurious upstream propagation of the eddy viscosity into attached laminar regions. In addition, recent updates by Spalart et al. [28] termed DDES (delayed detached eddy simulation) have been incorporated to enhance the ability of the model to distinguish between LES and RANS regions.

Spalart-Allmaras Detached Eddy Properties

Deformation Option

Selects the modified or standard production term.

 

Modified

Selects the modified production term. This is recommended for most simulations. See Eqn. 175.

 

Original

Selects the standard production term. This option allows comparison with results from other CFD codes that lack the modified production term. See Eqn. (173).

     

Convection

For guidance on selecting a convection, see Diffusion Term .

 

1st-order

Selects the first-order convection.

 

2nd-order

Selects the second-order convection.

Spalart-Allmaras Detached Eddy Expert Properties

Unless you are thoroughly familiar with the theoretical aspects of this model and the discretization techniques used in STAR-CCM+, we recommend that you not make any changes within the Expert category. The values in that category reflect both the model's design and discretization approaches that have been optimized for accuracy and performance. Tampering with them may diminish the effectiveness of the model.

     

Cb1

The coefficient , Eqn. 165.

     

Cb2

The coefficient , Eqn. 164.

     

Cdes

The DES length scale coefficient . Eqn. 183

     

CdesTimeLim

The DES blended upwind scheme time scale coefficient . Eqn. 183

     

Cprod

The coefficient , Eqn. 175.

     

Cv1

The coefficient , Eqn. 171.

     

Cv2

The coefficient , Eqn. 169.

     

Cw2

The coefficient , Eqn. 180.

     

Cw3

The coefficient , Eqn. 179.

     

Kappa

The von Karman constant , Eqns.(168) and (181).

     

Low Re Correction

Option to include the low Reynolds number correction factor in Eqn. 183. If checked, is computed as in Eqn. 186. If unchecked, is set to 1.

     

Secondary Gradients

Neglect or include the boundary secondary gradients for diffusion and/or the interior secondary gradients at mesh faces.

 

On

Include both secondary gradients.

 

Off

Exclude both secondary gradients.

 

Interior Only

Include the interior secondary gradients only.

 

Boundaries Only

Include the boundary secondary gradients only.

     

Sigma

The coefficient , Eqn. 164.

Field Functions Reference

The following primitive field functions are made available to the simulation when the Spalart-Allmaras turbulence model is used. These objects all have the same base properties.

DES Low Re Correction Factor

The low-Reynolds number correction function defined in Eqn. 186

   

DES Upwind Blending Factor

The blending function for the hybrid upwind scheme

   

Detached Eddy Length Scale

The cell length scale used for detached eddy simulation , see Eqn. 183.

   

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