The Segregated Flow model solves the flow equations (one for each component of velocity, and one for pressure) in a segregated, or uncoupled, manner. The linkage between the momentum and continuity equations is achieved with a predictor-corrector approach.
The complete formulation can be described as using a colocated variable arrangement (as opposed to staggered) and a Rhie-and-Chow-type pressure-velocity coupling combined with a SIMPLE-type algorithm.
This model has its roots in constant-density flows. Although it is capable of handling mildly compressible flows and low Raleigh number natural convection, it is not suitable for shock-capturing, high Mach number and high Raleigh-number applications.
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Selects the convection scheme to be used. |
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| 1st-order |
Selects the first-order upwind convection scheme. |
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| 2nd-order |
Selects the second-order upwind convection scheme. |
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| Central |
Selects the central difference convection scheme (available with large eddy simulation (LES) only). |
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| DES Hybrid |
Selects the hybrid second-order upwind/central scheme (available with detached eddy simulation (DES) only). |
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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.
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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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