The conservation of mass (water) equation results in the PDE
$a\frac{\partial j}{\partial x} - \frac{\partial D_{sz}}{\partial t} = i - j$ (1)
where
$i$ | = | input from unsaturated zone |
$a$ | = | upstream area per unit boundary length draining through the element |
$D_{sz}$ | = | saturation zone deficit, and |
$j$ | = | $q_{sz}$ (outflow) |
The following three assumptions make the solution of Equation (1) simpler.
Under these assumptions the saturated zone flow $q_{sz}$ can be shown to be:
$q_{sz} = j = \frac{\sigma}{a} T_0 e^{-D_{sz}/m}$ (2)