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> | ||
- | we have <br> | + | For continuity we have <br> |
- | :<math> \ | + | :<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> | |
- | : | + | :<math> H = \sum\limits_{neighbours} {a_l } \vec v_l </math> <br> |
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- | + | This interpolation of variables H and <math> {\nabla p} </math> based on coefficients <math> a_p </math> for [[Velocity-pressure coupling | pressure velocity coupling ]] is called <b>Rhie-Chow interpolation</b>. | |
+ | |||
+ | the Rhie-Chow interpolation is the same as adding a pressure term, which is proportional to a third derivative of the pressue | ||
+ | |||
+ | ---- | ||
+ | <i> Return to: <br> | ||
+ | # [[Numerical methods | Numerical Methods]] | ||
+ | # [[Solution of Navier-Stokes equation]] | ||
+ | </i> |
Latest revision as of 06:14, 27 August 2012
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.
the Rhie-Chow interpolation is the same as adding a pressure term, which is proportional to a third derivative of the pressue
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