The Coupled Flow model solves the conservation equations for mass and momentum simultaneously using a time- (or pseudo-time-) marching approach. The preconditioned form of the governing equations used by the Coupled Flow model makes it suitable for solving incompressible and isothermal flows.
One advantage of this formulation is its robustness for solving flows with dominant source terms, such as rotation. Another advantage of the coupled solver is that CPU time scales linearly with cell count; in other words, the convergence rate does not deteriorate as the mesh is refined.
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Selects the integration scheme to use. |
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| Implicit |
The coupled implicit solver will be invoked. Adds a Coupled Implicit node to the Solvers node. |
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| Explicit |
The coupled explicit solver will be invoked. Adds a Coupled Explicit node to the Solvers node. |
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Selects the discretization scheme to be used. |
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| 1st-order |
Selects the first-order upwind discretization scheme |
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| 2nd-order |
Selects the second-order upwind discretization scheme. |
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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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Minimum allowable absolute pressure. |
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Maximum rate that temperature is allowed to increase. |
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Enable/disable preconditioning. |
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| Ticked |
Enable preconditioning. |
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| Cleared |
Disable preconditioning. |
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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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