Efficient multi-scale finite element method for simulating two-dimension water flow movement in porous media
A porous medium, finite element technology, applied in the field of hydraulics, can solve the problem of high consumption of basis function construction, and achieve the effects of reduced calculation time, simple principle and high unit flexibility
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Embodiment 1
[0055] Example 1: Continuum model of two-dimensional steady flow
[0056] The research area is a square area: Ω=[50m, 150m]×[50m, 150m], permeability coefficient K(x,y)=x 2 m / d, the research equation is the steady flow equation:
[0057] ∂ ∂ x ( K ∂ H ∂ x ) + ∂ ∂ y ( K ∂ H ∂ y ) = 0 ,
[0058] Boundary condition is constant head boundary condition The source-sink item is 0, and this model has an analytical solution: H=x 2 -3y 2 .
[0059] Sub-example 1.1: Solved using LFEM, LFEM-F, MSFEM-L...
Embodiment 2
[0066] Example 2: Gradient medium model of two-dimensional unsteady flow
[0067] The research area is a square area: Ω=[0,10km]×[0m,10km], the research equation is:
[0068] S ∂ H ∂ t - ∂ ∂ x ( K ∂ H ∂ x ) - ∂ ∂ y ( K ∂ H ∂ y ) = W ,
[0069] The thickness of the aquifer in the study area is 10m, and the left and right sides are the boundaries of constant water head, the water heads a...
Embodiment 3
[0078] Embodiment 3: two-dimensional submerged flow model (non-linear model)
[0079] The research equation is the Boussinesq equation:
[0080] - ▿ · K ( x , y , H ) ▿ H = W ,
[0081] All parameters in this example have been dimensionless and have no units; the study area is: Ω=[0,1]×[0,1], the boundary water head is the boundary of constant head and both are 0, the base level b=-4, the permeability coefficient for:
[0082] K ( x , y , H ) = T ( H - b ) ...
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