Page 158 - Percolation Models for Transport in Porous Media With
P. 158

154          CHAPTER 8.  CONDUCTIVITY AND ELECTRIC CURRENT















                             ~~-----++------~~~--~t~gt~/~
         Figure 56:  Variation of the permeability of the medium depending on the duration
         of treatment with periodic current


         starting from  t;::: Tq(rl)  the r1-chain begins to conduct.  The function  F2(rt,R,t)
         depends on its argument rather weakly  and is  close  to Fo(rl).  Therefore,  after
         setting  R = rz,  t = To(rl),  we  can  obtain  the following  value  from  (8.25)  with
         good accuracy
                                  Tq(r!)  ~ t(rt, rz, To(rl))

            The relationship (8.22), with regard to the condition (8.21}, shows that To(rt)
         decreases  rapidly  as  r1 grows  (perhaps,  with  small  violations  of monotonicity),
         while Tq(rl)  > To(r1) and decreases more rapidly than To(rtO as r1  grows.  There-
         fore  the  thick  rz-chains  are the first  of all  r1-chains  to become  conducting and
         increase the electric conductivity, and a*-chains are the last to do so.  This results
         in the conservation of the initial hierarchy of r1-chains with respect to the values
         of their average electric conductivity during the electric treatment.
            It follows  from  (8.21),  (8.25)  that for  the "temperature mechanism"  R(rt,t)
         grows slower than In t, while for the "gradient mechanism" R(rt, t) is upper bounded.
         If we  also take into account the fact  that large capillaries affect  the average hy-
         draulic and electric conductivity of an r1-chain to a small degree, we can notice that
         as time passes, K(t) and I;(t)  steady.  (According to (8.18), the major contribu-
         tion to the alteration ofthe specific electric conductivity I;(t) and the permeability
         K(t) of the medium is made by the thick r1-chains.)
            We shall proceed to determine the starting time t' for  changes of I; and K  in
         the medium and the time t" when these changes stop

                     t'(Eo) = min(To(rt,Eo)),  t"(Eo) = max{Tq(rt.Eo))     (8.26)

            Here the minimum and maximum are taken over all non-conducting r1-chains
         (a*  :5  r1  :5 rz).
            Results of the numerical calculation of K(t) for  a function  of the form  (8.19)
         and the same values of the parameters as in §8.2, are presented in fig.  56.
   153   154   155   156   157   158   159   160   161   162   163