Steady-State Topography-Driven FlowDeveloped by Paul Hsieh, USGSSkip ahead to run the modelIntroductionA topography-driven flow system is one in which ground water flows from higher-elevation recharge areas (where hydraulic head is higher) to lower-elevation discharge areas (where hydraulic head is lower). See figure below. The boundaries of the flow domain are as follows:
The no-flow boundaries might represent low-permeability bedrock that bounds the basin. Alternatively, the vertical boundaries might also represent ground-water flow divides. Important Note: 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 steady state. Governing EquationThe steady-state ground-water flow equation to be solved is where h is hydraulic head, and Kxx and Kzz are the principal values of the hydraulic conductor tensor. The principal directions are assumed to be parallel to the xand z axes. Boundary ConditionsAssuming we know the position of the water table, 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 After solving for hydraulic head h, the x and z components of the linear 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.
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