Page 173 - Fundamentals of Computational Geoscience Numerical Methods and Algorithms
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7.3  Verification and Application of the Equivalent Source Algorithm  163

              Due to the geometrical symmetry of the ideal experiment, analytical solutions
            for the temperature distribution during the solidification of the intruded magma can
            be expressed as follows.


                                                   √
                                            L M
                       T R = T m    0 ≤ x ≤    − 2β αt, t ≤ t MMax ,     (7.21)
                                            2
                                                             √
                                                2x + L M − 4β αt

                                  (T m − T R0 )erfc    √
                                                      4 αt
                        T R = T R0 +
                                              1 + erf(β)                 (7.22)

                                  L M     √
                                      − 2β αt ≤ x ≤ L R , t ≤ t MMax ,
                                   2
                               )               *
                         ρ M L M c pM (T m − T R0 ) + L  x 2
              T R = T R0 +           √          e −  4αt    ( t > t MMax ),  (7.23)
                               2ρ R c pR απt
            where erfc(x) = 1 − erf(x) is the complementary error function of variable x;
                            2
            t MMax = L  2  " (16αβ ) is the maximum time instant to complete the solidification
                     M
            of the intruded magma.
              In summary, the proposed equivalent algorithm for simulating the chemical effect
            of the intruded magma solidification includes the following five main steps: (1) For
            the given values of the initial temperature of the rock, T R0 , and the solidification
            temperature of the intruded magma, T m , Eq. (7.17) is solved to determine the value
            of β; (2) Substituting the value of β into Eq. (7.20) yields the value of the phys-
            ically equivalent heat source due to the solidification of the dike-like and sill-like
            intruded magma; (3) Eqs. (7.12) and (7.15) are used to calculate the mass source of
            the released volatile fluids during the intruded magma solidification; (4) The inte-
            gration time step is determined using Eqs. (7.15) and (7.16); (5) The conventional
            finite element method is used to solve Eqs. (7.6) and (7.7) for the temperature and
            concentration distribution in the whole domain during and after solidification of the
            intruded magma. Note that both the mass source and the physically equivalent heat
            source are only applied to some elements in the finite element analysis during the
            solidification process of the intruded magma. The automatic transition from solid-
            ification to post-solidification of the intruded magma is another advantage in using
            the proposed equivalent source algorithm for simulating the chemical effect of the
            intruded magma solidification in the conventional finite element analysis.


            7.3 Verification and Application of the Equivalent
                Source Algorithm

            Since the key part of the proposed algorithm for simulating the chemical effect of the
            intruded magma during solidification is to transform the original moving interface
            (i.e. the solidification interface between the rock and intruded magma) problem into
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