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5.1  Mathematical Background of Chemical Dissolution Front Instability Problems  107

            where
                                        ψ(φ 0 )  k(φ 0 )
                                    β =       =      ,                   (5.67)
                                        ψ(φ f )  k(φ f )

                                      %
                                            2
                                                 2
                                        (p ) + 4m − p

                                          fx          fx
                                  σ =                  .                 (5.68)
                                              2
              Substituting Eq. (5.66) into Eq. (5.64) yields the following equation for the
            growth rate of the small perturbation:
                            −p              %
                               fx                 2     2


                ω(m) =               [−p −    (p ) + 4m + (1 − β) |m|).  (5.69)
                                                fx
                                         fx
                       (1 + β)(φ f − φ 0 )
              Equation (5.69) clearly indicates that the planar dissolution front of the reactive
            transport system, which is described by the above-mentioned second special prob-
            lem, is stable to short wavelength (i.e. large wavenumber m) perturbations but it is
            unstable to long wavelength (i.e. small wavenumber m) perturbations.
              Letting ω(m) = 0 yields the following critical condition, under which the reac-
            tive transport system can become unstable.
                                            (3 − β)(1 + β)
                                   &
                                 p    &  =−              ,               (5.70)
                                  fx critical
                                               2(1 − β)
                    &
            where p    &  is the critical value of the generalized dimensionless pressure gra-
                   fx critical
            dient in the far upstream direction as x approaching negative infinite (Zhao et al.
                          &
            2008e). Since p    &  is usually of a negative value, the following critical Zhao
                         fx critical
            number is defined to judge the instability of the reactive transport system:
                                                 (3 − β)(1 + β)
                                          &
                            Zh critical =−p    &  =           .          (5.71)
                                        fx critical
                                                    2(1 − β)
              Thus, the Zhao number of the reactive transport system can be defined as follows:

                                          ∗
                           p L  ∗   k(φ f )L p

                            fx              fx     v flow        V p
             Zh =−p =−          =−                                     . (5.72)
                     fx                       =
                            p ∗     φ f μD(φ f )  φ f D(φ f )  k chemical A p C eq
              Using Eqs. (5.71) and (5.72), a criterion can be established to judge the instability
            of a chemical dissolution front associated with the particular chemical system in this
            investigation. If Zh > Zh critical , then the chemical dissolution front of the reactive
            transport system becomes unstable, while if Zh < Zh critical , then the chemical dis-
            solution front of the reactive transport system is stable. The case of Zh = Zh critical
            represents a situation where the chemical dissolution front of the reactive transport
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