Potential flow terms

The potential flow is calculated using Darcy's law

(30.2)   SZ_TechnicalReference00004.jpg

where Dh is the piezometric head difference and C is the conductance.

The horizontal conductance in Eq. (30.2) is derived from the harmonic mean of the horizontal conductivity and the geometric mean of the layer thickness. Thus, the horizontal conductance between node i and node i-1 will be

(30.3)   SZ_TechnicalReference00007.jpg

where, KH is the horizontal hydraulic conductivity of the cell and Dz is the sat­urated layer thickness of the cell.

The vertical conductance between two cells is computed as a weighted serial connection of the hydraulic conductivity, calculated from the middle of layer k to the middle of the layer k+1. Thus,

(30.4)   SZ_TechnicalReference00010.jpg

where Dz is the layer thickness

Dewatering conditions

Consider the situation in Figure 30.1, where the cell below becomes dewa­tered.

dewatering_below.jpg 

Figure 30.1        Dewatering conditions in a lower cell.

The actual flow between cell k and k+1 is

(30.5)   SZ_TechnicalReference00013.jpg

In the present solution scheme the flow will be computed as

(30.6)   SZ_TechnicalReference00016.jpg

Subtracting Eqs.(30.5) from (30.6) gives the correction term

(30.7)   SZ_TechnicalReference00019.jpg

which is added to the right-hand side of the finite difference equation using the last computed head.

A correction must also be applied to the finite difference equation if the cell above becomes dewatered.

dewatering_above.jpg 

Figure 30.2        Dewatering conditions in the cell above

Thus, from Figure 30.2, the flow from cell k-1 to k is

(30.8)   SZ_TechnicalReference00022.jpg

where, again the computed flow is

(30.9)   SZ_TechnicalReference00025.jpg

Subtracting Eqs. (30.8) from (30.9) gives the correction term

(30.10)   SZ_TechnicalReference00028.jpg

which is added to the right-hand side of the finite difference equation using the last computed head