Page 172 - Fundamentals of Computational Geoscience Numerical Methods and Algorithms
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162  7  Simulating Thermal and Chemical Effects of Intruded Magma Solidification Problems

              The time, at which the intruded magma solidification boundary reaches both
            sides of the kth finite element boundary in the magma solidification direction, can
            be determined from the analytical solution (Carslaw and Jaeger 1959).

                                            2
                    2
                   k (Δx) 2           (k − 1) (Δx) 2
             t Mk =       ,    t Mk−1 =                   (k = 1, 2, 3, ..., K),
                    4αβ 2                 4αβ 2
                                                                         (7.16)
                       "
            where α = λ R (ρ R c pR ) is the thermal diffusivity of the rock; β can be determined
            from the following transcendental equation:
                                                   √
                                   e −β 2        L π
                                           =              ,              (7.17)
                                β[1 + erf(β)]  c pR (T m − T R0 )
            where T R0 is the initial temperature of the rock; erf(β) is the error function of vari-
            able β.

                                           2     β  −r  2
                                   erf(β) = √    e   dr.                 (7.18)
                                            π  0
              Substituting Eqs. (7.14) into Eq. (7.13) yields the following equation:

                                     ρ M L
                        f (x, y, t Mk ) =        (k = 1, 2, 3,..., K).   (7.19)
                                     Δt Mk

              Finally, substituting Eq. (7.16) into Eq. (7.19) yields the following equation:

                                4ρ M Lαβ  2
                 f (x, y, t Mk ) =       2        (k = 1, 2, 3,. . . , K),  (7.20)
                              (2 k − 1)(Δx)
                                 "
            where Δx = ΔL Mk = L M (2K) and ΔL Mk is the constant solidification thickness
            of the intruded magma during the variable time period Δt Mk .
              It needs to be pointed out that since the magma solidification boundary passes
            only through the kth finite element from the initial intruded interface between the
            rock and magma during the time period Δt Mk , both the mass source of the released
            volatile fluids and the physically equivalent heat source expressed in Eqs. (7.12) and
            (7.20) only need to be applied in the kth finite element, which is numbered from the
            initial intruded interface between the rock and magma, in the finite element analysis.
            This means that if a fixed finite element mesh is employed, the variable time step
            expressed by Eqs. (7.15) and (7.16) needs to be used during the magma solidification
            period in the finite element analysis. From the numerical analysis point of view, a
            change in the time step is much easier to implement than a change in the finite
            element mesh in the finite element analysis. This is the main advantage in using the
            proposed equivalent source algorithm to simulate the chemical effect of the intruded
            magma solidification in geological systems.
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