Page 29 - Percolation Models for Transport in Porous Media With
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20                                CHAPTER 1.  PERCOLATION MODEL

         which satisfy the condition 0'1 (O)  :::;  u  :::;  0'1 (t) have already had their conductivities
         changed.)  To obtain the condition for the conductivity change, define the energy
         discharge t:1  in the bond u 1 (t)  contained in the chain u1 (0).  After neglecting the
         effects  of heat exchange between the chains and the non-conducting skeleton of
         the medium, we obtain


                         2
                                        2
                       E
                                                   (  ))
                                       E It  2(
                                (  ))
               0'1(t)
                            2(
             E -- = -(-) l;  0'1  0  + -(t)   l;  0'1  T  dr,               (1.18)
                O'm   0'1  t          0'1
                                           to
            The first term in the right side of the relationship (1.18) corresponds to Joule's
         heat  which  has  discharged  in  the  bond  before  the  instant  to  =  eu;, 1
         x  (''Vr/J*)- 2 ,  when  the  conductivity  of the chain  began  to change.  The second
         term describes the energy discharge during the period when  the conductivity of
         the chain was changing.  In this case,  t~c  is the time needed for all elements of the
         chain to acquire infinite conductivity.
            Consider the change of the conductivity in the case when the probability density
         f 0(u) of the bonds with respect to intrinsic conductivities is described by the model
         function
                                                                            (1.19)

            In this case the solution (1.18) can be obtained in the analytical form.  As it can
         be deduced from the relationship (1.16), the value 'ilr/J* f E = nf(n -1) is the same
         for all chains and is assumed at those bonds which have the least conductivity for
         the given chain.
            For an arbitrary chain,  (1.18)  implies

                                                                   1
                                                           An= 2(n -1)

            This  means  that  according  to  (1.9),  the  average  conductivity  of all  chains
         increases  in  the like  fashion,  i.e.,  proportional to 1- (n- 1)(tft0  - 1)-~"n, so
         that  to  is  the  same  for  all  chains.  Therefore  the  effective  conductivity  of the
                        ITl
         medium I: (t) "' J I:(u(t)) du, and after integrating
                  0
                        0





            H bonds are cylindrical capillaries, then the electric conductivity u  of such a
         bond is related to its permeability coefficient k in the following way, k "' u 2 •  Thus
         we obtain the time dependence of the permeability K(t) of the medium

                       K(t)fK(O) = [1- (n -1)(tfto- 1)17(t- to)t ~nn
                                                               2
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