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