Rhie-Chow interpolation
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we have at each cell descretised equation in this form, <br> | we have at each cell descretised equation in this form, <br> | ||
:<math> a_p \vec v_P = \sum\limits_{neighbours} {a_l } \vec v_l - \frac{{\nabla p}}{V} </math> ; <br> | :<math> a_p \vec v_P = \sum\limits_{neighbours} {a_l } \vec v_l - \frac{{\nabla p}}{V} </math> ; <br> | ||
- | :<math> \left[ {\frac{1}{{a_p }}H} \right]_{face} = \left[ {\frac{1}{{a_p }}\frac{{\nabla p}}{V}} \right]_{face} </math> <br> | + | For continuity we have <br> |
+ | :<math> \sum\limits_{faces} \left[ {\frac{1}{{a_p }}H} \right]_{face} = \sum\limits_{faces} \left[ {\frac{1}{{a_p }}\frac{{\nabla p}}{V}} \right]_{face} </math> <br> | ||
where <br> | where <br> |
Revision as of 05:51, 24 October 2005
we have at each cell descretised equation in this form,
- ;
For continuity we have
where
This interpolation of variables H and based on coefficients for pressure velocity coupling is called Rhie-Chow interpolation.
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