Near-wall treatment for k-epsilon models
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Depending heavily on the problem description and the main quantity solution based on, the k-e model is influenced by the user to capture the phisical phonomena. heat transfer problems, high mach numbers with thin attached layers, low mach number with separations and heavy back flows ...etc. alle these different combinations requires an experimented user to define the priority and the solution dependency value. | Depending heavily on the problem description and the main quantity solution based on, the k-e model is influenced by the user to capture the phisical phonomena. heat transfer problems, high mach numbers with thin attached layers, low mach number with separations and heavy back flows ...etc. alle these different combinations requires an experimented user to define the priority and the solution dependency value. | ||
| - | [[ | + | [[Near-wall treatment for heat transfert dominated problems]] |
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| + | [[Near-wall treatment for low mach numbers dominated problems]] | ||
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| + | [[Near-wall treatment for high mach numbers dominated problems]] | ||
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| + | [[Near-wall treatment, influence of Reynolds number]] | ||
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Revision as of 22:40, 8 May 2006
Depending heavily on the problem description and the main quantity solution based on, the k-e model is influenced by the user to capture the phisical phonomena. heat transfer problems, high mach numbers with thin attached layers, low mach number with separations and heavy back flows ...etc. alle these different combinations requires an experimented user to define the priority and the solution dependency value.
Near-wall treatment for heat transfert dominated problems
Near-wall treatment for low mach numbers dominated problems
Near-wall treatment for high mach numbers dominated problems
Near-wall treatment, influence of Reynolds number
