Download SWAP version 3.2 Theory description and user manual
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Head controlled bottom boundary ∂Fn ∂hnj +1, p = Δz n Δt j −κ C nj +1 + Δz n ∂S mj +,n1 + ∂hnj +1 K j +κ K nj−+½κ + n+½ ½ (Δz n−1 + Δz n ) ½ Δz n j +κ ⎞ ∂K nj−+½κ ⎛⎜ hnj−+11 − hnj +1 ⎟ + κ ∂K n+½ 1 + ∂hnj +1 ∂hnj +1 ⎜⎝ ½ (Δz n−1 + Δz n ) ⎟⎠ ⎛ hnj +1 − hbot ⎞ ⎜ + 1⎟ ⎜ ½ Δz ⎟ n ⎝ ⎠ Predefined groundwater levels ∂S mj +, n1* ∂K nj*+−κ½ K nj*+−κ½ ∂Fi Δzi j +1 = + −κ C * + Δz n * ∂hnj*+1 Δt j n ∂hnj*+1 ½ ( Δz n * −1 + Δz n * ) ∂hnj*+1 ∂K nj*++κ½ K nj*++κ½ ⎛ z * − z n * +1 ⎞ ⎟ +⎜ n +κ ⎜ ⎟ ∂hnj*+1 ⎝ z n * − gwl ⎠ ½ (Δz n * + Δz n * +1 ) ⎛ h j*+1 − h j*+1 ⎞ ⎜ n −1 n + 1⎟ ⎜ ½ ( Δz * + Δz * ) ⎟ n −1 n ⎝ ⎠ ⎛⎛ z * − z * ⎞ ⎞ hnj*+1 ⎜⎜ n n +1 ⎟ + 1⎟ ⎜ ⎜ z * − gwl ⎟ ½ (Δz * + Δz * ) ⎟ n n +1 ⎠ ⎝⎝ n ⎠ Cauchy relation for the bottom boundary ∂Fn ∂hnj +1, p = Δz n Δt j −κ Cnj +1 + Δz n ∂S mj +,n1 + ∂hnj +1 K nj−+½κ K nj++½κ + ½ (Δz n−1 + Δz n ) ½ Δz n + cK nj++½κ j +κ ⎛ j +1 ⎞ ⎞ ∂K nj−+½κ ⎛⎜ hnj−+11 − hnj +1 ⎟ + κ ∂K n+½ ½ Δz n ⎜ hn − (ϕ − z n ) ⎟ 1 + ⎜⎜ j +κ 2 ⎟ ⎟ ∂hnj +1 ∂hnj +1 ⎜⎝ ½ (Δz n−1 + Δz n ) ⎟⎠ ⎝ ½ Δz n + cK n+½ ⎠ ( ) Seepage face hnj +1 + ½ Δz n < 0 → ∂F1 ∂h1j +1 = Δz1 Δt j C1j +1 + Δz1 ∂S mj +,11 ∂h1j +1 + ∂K j +κ K1j½+κ + κ 1j½+1 ½ (Δz i + Δzi +1 ) ∂h1 ∂Fn hnj +1 + ½ Δz n </ 0 → ∂hnj +1, p = Δz n Δt j −κ C nj +1 + Δz n ⎛ h1j +1 − h2j +1 ⎞ ⎜ + 1⎟ ⎜ ½(Δz1 + Δz 2 ) ⎟ ⎝ ⎠ ∂S mj +,n1 ∂hnj +1 + K nj−+½κ K j +κ + n+½ ½ (Δz n−1 + Δz n ) ½ Δz n j +κ ⎞ ∂K nj−+½κ ⎛⎜ hnj−+11 − hnj +1 ⎟ + κ ∂K n+½ 1 + ∂hnj +1 ∂hnj +1 ⎜⎝ ½ (Δz n−1 + Δz n ) ⎟⎠ ⎞ ⎛ hnj +1 ⎜ + 1⎟ ⎟ ⎜ ½ Δz n ⎠ ⎝ Free drainage ∂Fn ∂hnj +1, p = Δz n Δt j −κ Cnj +1 + Δz n ∂S mj +,n1 ∂hnj +1 + K nj−+½κ K j +1 + n+½ ½ (Δz n−1 + Δz n ) ½ Δz n j +1 ⎞ ∂K nj−+½κ ⎛⎜ hnj−+11 − hnj +1 ⎟ + κ ∂K n+½ 1 + ∂hnj +1 ∂hnj +1 ⎜⎝ ½ (Δz n−1 + Δz n ) ⎟⎠ The internodal conductivity K nj++½1 is in the case of free drainage irrespective the value of κ always treated implicitly 236 Alterra Report 1649 - 01