Second order partial differential equation of parabolic type on the space-time field variable :
\beta({\bf r}, U) \cdot \frac{\partial U}{\partial t} = \nabla \left( \alpha({\bf r}, U) \nabla U \right) + f({\bf r}) |
where
space-time field variable | mobility kinetic coefficient | ||
time | capacitance kinetic coefficient | ||
Position vector | density of external forces |
In the absence of external forces and constant kinetic coefficients the diffusion equation takes form:
\frac{\partial U}{\partial t} = D \cdot \Delta U + f({\bf r}) |
where is called the diffusion coefficient.