Page 114 - Percolation Models for Transport in Porous Media With
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6.1  MERCURY INJECTION                                               107

         mercury [75].
            The initial  stage of displacement.  Suppose that at the initial stage dis-
         placement  takes  place  along  non-intersecting  tortuous  paths.  In  this  case  the
         fraction of the super-critical capillaries being filled  with mercury is
                                                   00
                               X(rk) = 1- F(rk) = J f(r) dr.                 (6.2)
                                                  rk
            The probability {i of the first i capillaries being super-critical and the ( i + 1 )-th
         capillary having radius rk  (i.e., subcritical) is  Xi(rk) F(rk)·
            The average volume  v'(rk)  of a super-critical capillary is  found  as the condi-
         tional expectation of the random variable 1rr 2 l  (capillary volume)  when rk  :::;  r <
         oo.  The volume of mercury that has reached the first i  super-critical capillaries in
         a chain equals iv'(rk)·  After averaging this volume with regard to the expression
         for  probability {i, we obtain the mean volume V(rk) of mercury which has passed
         into the chain of total volume V  =  V(rk  =  0).  Since at the considered stage the
         saturation of the pore space with mercury isS= V(rk)/V, using (6.2) we obtain
         the following correlation

                                                                             (6.3)



         After  using  (6.1)  to  pass  to  the  variable  rk,  in  the  dependence  S(LlP),  which
         has been  measured  by  means of the  mercury porometry method,  we  obtain the
         experimentally determined dependence S(rk).
            After integrating the right side of (6.3)  by parts using (6.2) and then differen-
         tiating both sides of the obtained equation with respect to rk, we obtain

                                                                             (6.4)


            After passing in (6.4) to the new independent variableS we obtain an ordinary
         differential equation for the function X(S) with the initial condition X(S =  0) = 0.
                           X(S) = 1 -ex+ I s• : ~;;l(S') l                   (6.5)
         Its solution is

                                                v


         From  (6.5)  and  (6.2)  we  obtain  the  desired  dependence  f(rk)  =  -(1
         - X)V(V S + 1rlrn- 1 (dSjdrk).
            At  the instant when  mercury appears in  the outer cross-section,  the fraction
         X  of the super-critical pores equals the percolation threshold Xc,  and an infinite
         cluster of the super-critical poresis formed.  The value Xc  is determined from  the
         relationship (1.1).
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