sunfluidh:sunfluidh_link_equations_data_set
Différences
Ci-dessous, les différences entre deux révisions de la page.
Les deux révisions précédentesRévision précédenteProchaine révision | Révision précédenteDernière révisionLes deux révisions suivantes | ||
sunfluidh:sunfluidh_link_equations_data_set [2016/11/30 14:31] – [Links equations & Data set] yann | sunfluidh:sunfluidh_link_equations_data_set [2018/12/17 14:56] – [The different formulations of the Poisson's equation] yann | ||
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Ligne 13: | Ligne 13: | ||
$$ \vec{V}^{n+1}= \vec{V}^* - \frac{\Delta t}{\rho} \nabla \phi$$ | $$ \vec{V}^{n+1}= \vec{V}^* - \frac{\Delta t}{\rho} \nabla \phi$$ | ||
- | For more details on the projection methods, see the document on the numerical methods used in Sunfluidh [[sunfluidh: | + | **For more details on the projection methods, see the document on the numerical methods used in Sunfluidh [[sunfluidh: |
</ | </ | ||
Ligne 64: | Ligne 64: | ||
<note important> | <note important> | ||
- | We remind the user that the low Mach hypothesis is based on the hypothesis of the scale splitting between the thermodynamics and dynamics phenomena. As a consequence the pressure is read as $P= P_{th}+P_{dyn}$, | + | We remind the user that the low Mach hypothesis is based on the hypothesis of the scale splitting between the thermodynamics and dynamics phenomena. As a consequence the pressure is read as $P= P_{th}+P_{dyn}$, |
</ | </ | ||
Ligne 111: | Ligne 111: | ||
[[sunfluidh: | [[sunfluidh: | ||
+ | |||
+ | <WRAP info> | ||
+ | **Information on numerical methods used for solving these equations is available in the pdf document present [[ : | ||
+ | </ | ||
+ | |||
===== Link between the data set & the variables in equations ===== | ===== Link between the data set & the variables in equations ===== |
sunfluidh/sunfluidh_link_equations_data_set.txt · Dernière modification : 2018/12/17 14:58 de yann