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.
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Selects the modified or standard production term. |
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| Modified |
Selects the modified production term. This is recommended for most simulations. See Eqn. 175. |
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| 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). |
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For guidance on selecting a convection, see Diffusion Term . |
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| 1st-order |
Selects the first-order convection. |
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| 2nd-order |
Selects the second-order convection. |
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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.
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The coefficient |
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The coefficient |
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The DES length scale coefficient |
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The DES blended upwind scheme time scale coefficient |
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The coefficient |
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The coefficient |
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The coefficient |
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The coefficient |
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The coefficient |
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Option to include the low Reynolds number correction factor |
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Neglect or include the boundary secondary gradients for diffusion and/or the interior secondary gradients at mesh faces. |
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| On |
Include both secondary gradients. |
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| Off |
Exclude both secondary gradients. |
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| Interior Only |
Include the interior secondary gradients only. |
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| Boundaries Only |
Include the boundary secondary gradients only. |
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The coefficient |
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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.
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The low-Reynolds number correction function |
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The blending function for the hybrid upwind scheme |
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The cell length scale used for detached eddy simulation |