For a two-dimensional vertical section, the boundaries of the flow domain are as follows:
The top boundary (AB) is the water table, which is assumed to lie close to land surface.
The two vertical boundaries (BC and AD) and the bottom boundary (DC) are no-flow boundaries.
The no-flow boundaries might represent groundwater flow divides or low hydraulic conductivity bedrock that bounds the basin.
Note that by specifying the position of the water table, it is assumed that the pattern of recharge and discharge is such that the water table is maintained at a steady state.
Steady-state flow of ground water in the vertical section is governed by the equation
where h is hydraulic head, and Kxx and Kzz are the principal values of the hydraulic conductivity tensor. The principal directions are assumed to be parallel to the cartesian axes x and z.
Assuming the position of the water table is known, the boundary condition along the water table (AB) is
where z is the elevation of the water table.
Along the vertical boundaries BC and AD, the no-flow boundary condition is
Along bottom boundary CD, the no-flow boundary condition is
TopoDrive solves the above equations by the finite-element method.
The flow domain is represented by a deformed rectangular mesh, and each quadrilateral cell is divided into two triangular elements.
Linear basis functions are used to formulate the finite-element formulation.
After solving for hydraulic head h, the x and z components of the groundwater velocity vector are computed by
where n is porosity. The velocity vectors are used for calculating flow paths and the advective movement of fluid particles.