Lines Matching refs:rho

12 \rho &= \rho_\infty\left(1+A\exp\left(\frac{-(\bar{x}^2 + \bar{y}^2)}{2\sigma^2}\right)\right) \\
122 \begin{aligned} \rho &= \frac{P_0}{( c_p - c_v)\theta(\bm{x},t)} \pi(\bm{x},t)^{\frac{c_v}{ c_p - c…
389 \rho &= \frac{p}{R T_0} \\
423 \frac{\partial \rho}{\partial t} + \nabla \cdot \bm{U} &= 0 \\
424 \frac{\partial \bm{U}}{\partial t} + \nabla \cdot \left( \frac{\bm{U} \otimes \bm{U}}{\rho} + P \bm…
425 \frac{\partial E}{\partial t} + \nabla \cdot \left( \frac{(E + P)\bm{U}}{\rho} \right) &= 0 \, , \\
429 …te}`zhang2011verification`, the mean flow for this problem is $\rho=1$, $P=1$, $T=P/\rho= 1$ (Spec…
436 There is no perturbation in the entropy $S=P/\rho^\gamma$ ($\delta S=0)$.
477 …roblem. The default initial conditions are $P=1$, $\rho=1$ for the driver section and $P=0.1$, $\r…
494 \tau_{SHOCK} = \frac{h_{SHOCK}}{2u_{cha}} \left( \frac{ \,|\, \nabla \rho \,|\, h_{SHOCK}}{\rho_{re…
497 …ity gradient unit vector is defined as $\hat{\bm j} = \frac{\nabla \rho}{|\nabla \rho|}$. The orig…
545 …in HONEE for pure advection-diffusion, which holds density $\rho$ and momentum density $\rho \bm u…