Pressure diffusion with constant coefficients:
| \beta \, \frac{\partial p}{\partial t} = \nabla ( \alpha \nabla p) + q({\bf r}) |
where
| \frac{\partial \alpha({\bf r})}{\partial p} = 0 |
| \frac{\partial \beta({\bf r})}{\partial p} = 0 |
It honours linear PDE
Pressure diffusion with constant coefficients:
| \beta \, \frac{\partial p}{\partial t} = \nabla ( \alpha \nabla p) + q({\bf r}) |
where
| \frac{\partial \alpha({\bf r})}{\partial p} = 0 |
| \frac{\partial \beta({\bf r})}{\partial p} = 0 |
It honours linear PDE