The quadratic pressure-strain model of Sarkar, Speziale and Gatski [50] is a more modern formulation. The node of this model has its own properties.
This model can only be used with a high-
wall treatment (that is, using wall functions) without resolving the viscous-affected region.
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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 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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The coefficient |
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The coefficient |
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Determines how the coefficient |
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| None |
Neglects the term |
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| Boundary Layer Orientation |
Computes |
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| Thermal Stratification |
Computes |
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The coefficient |
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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 coefficient |
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The minimum value that the transported variable |
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The minimum value that the transported variable |
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| Use Boussinesq Approximation |
Instead of using the divergence of the computed Reynolds-stress tensor, use the Boussinesq approximation given by Eqn. 239. |
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| Ticked |
Use Boussinesq approximation. |
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| Cleared |
Use computed Reynolds stresses. |
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