Continuity equation Momentum equation...

Continuity equation	Momentum equation	Energy equation
$^{m + \frac{1}{2}} = p^{m p} - \frac{Δ t p}{2} ξ p^{m p} + \frac{1}{M a^{2}} (\nabla \cdot u^{m}) \leftarrow,^{m + 1} =^{m p} - Δ t p ξ p^{m + \frac{1}{2}} + p \frac{1}{M a^{2}} (\nabla \cdot u^{m}) \leftarrow$	$u^{m + \frac{1}{2}} = u^{m} + p \frac{Δ t p}{2 R e p} - Re (u^{m} \cdot \nabla) u^{m} + \nabla \cdot {\bar{t}}^{m p} - \nabla^{m}, u^{m + 1} = u^{m} + p \frac{Δ t p}{R e p} ((- R e p u^{m + \frac{1}{2}} \nabla u^{m + \frac{1}{2}} + \nabla \cdot {\bar{τ}}^{m + \frac{1}{2}} - \nabla^{m})) \cdot$	$T^{m + \frac{1}{2}} = T^{m} + p \frac{Δ t p}{2 P e p} - P e (u^{m} \cdot \nabla) T^{m} + \nabla^{2} T^{m} + B r ({\bar{τ}}^{m p} : p \nabla u^{m}), T^{m + 1} = T^{m} + p \frac{Δ t p}{P e p} - P e (u^{m} \cdot \nabla) T^{m + \frac{1}{2}} + \nabla^{2} T^{m + \frac{1}{2}} + B r ({\bar{τ}}^{m p} : p \nabla u^{m}) .$

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