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8.2  CONDUCTIVITY AND PERMEABILITY CHANGE I                          147

            Here Co  and Cb  depend on the form  of u(t) and are of the order unity each;

         "Yo  R:l  1.780 is the Euler- Masceroni constant.  It can be seen from  (8.9}  that as T
         grows, T' decreases quicker than T.
            Compare the energy density Wt  and amplitude It of a short impulse (r < Tk},
         when T'(rt) = T~ and (8.8}  holds, to the energy density w2 and amplitude I2 of a
         very long impulse (r2  ~ Tk},  when T(r} = Tc  and (8.9}  holds,






            For example,  for  Tt  = 10- 5  s,  T2  = 2 s,  Tk  = 2.5 · 10- 4  s  (for  r  = 10- 5  m,
         Kt = 10- 7  m 2  /s and T~ R:l  Tcr-t} we obtain w2/Wt  R:l  5 · 10 3 ,  I2/ It  R:l  0.16, i.e., if
         the "temperature mechanism" is realized, it is possible to decrease the amplitude of
         the impulse a little (by a factor of 5 to 10}.  At the same time, energy consumption
         grows by thousands of times, and the duration of impulse has to be increased by
         hundreds of thousands of times.  Thus impulse current with  short impulses  and
         a large amplitude, for  which  the "gradient"  mechanism of cement  destruction is
         realized, is the most effective one.
            The  dependence  of the  threshold  value  of the  current  amplitude  Ic  on  the
         capillary radius r for a fixed duration T  of impulse can be determined from formulas
         (8.4}  - (8.6}


                                                                            (8.10}



         8.2  Permeability and  Electric  Conductivity un-
                 der Impulse Current


         Consider  impulse  current  passing  through  an  element  of the  medium.  Current
         flows  both along "parallel"  rt-chains of the "skeleton of the infinite cluster"  and
         along bridges that connect  the rt-chains.  However  the current flowing  along rt-
         chains can  be calculated as  though  there are no  bridges,  since the allowances to
         the presence of these bridges, and consequently, the possible rearrangement of the
         current flow  in rt-chains, are insignificant according to the results of §1.2.
            Let the fraction of capillaries filled  with cement  be equal to K = 1 - K.  Fur-
                                                                   1
         thermore let all  these capillaries be thin,  i.e.,  K =< a*, 1, rz  >,  where  rz  is  the
                                                    1
         radius of the thickest capillary filled  with cement.
            All chains with a*$ r $  rz do not conduct.  We will further mark the quantities
         relating to the fluid  with  index  1,  and  those relating  to  the cement,  with  index
         2.  Using  the expressions  (3.1},  (8.1}  for  amplitude I 0(rt) of the current flowing
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