Page 165 - Percolation Models for Transport in Porous Media With
P. 165

162            CHAPTER 9  ELECTRIC ACTION EFFECT. EXPERIMENT






                                  •  1
                                  ~>2
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                          IQ




                           5
                                                      •
                                                 A  A  &
                            ····~·······~
                           0      42     4+     46     IJ,I   1.,"
         Figure 59:  Typical  dependence  1/ u y  =  f ( L) in  the electric  porometry experi-
         ments;  1,  2- measurements were  taken before and after electric treatment with
         impulse current, respectively


         treatment)  and  compared  to  the  initial  RJ(Li)·  In  the majority of cases  these
         values did not differ by more than 5%.
            Stage 4.  Electric treatment of the rock with  current of density j 0 ,  greater
         than  the  hypothetical  threshold  value ic,  was  carried  out  for  a  certain  period.
         Permeability of the specimen was being measured throughout the whole treatment.
         Furthermore after the electric treatment was terminated, these measurements were
         being taken for 2 to 7 more days, until the value of permeability steadied.
            Stage 5.  As at stage 2,  the values of u~(Li) and, correspondingly, f'(r), were
         determined.  The  results  of the  electric  treatment  of a  sandy-argillaceous  rock
         specimen  (see  table 9.1,  series I)  with  impulse current are presented in  figs.  59,
         60.
            It  is  clear  from  fig.  59  that  the electric  conductivity falls  rapidly  with  the
         increase of height.  Moreover after the electric treatment, the total conductivity of
         the column increases during the steady state flow through it and u~(L) falls more
         sharply with the increase of height L than does uy(L).
            Comparison of the curves f(r) and /'(r) presented in fig.  60, a, and marked by
         numbers 1 and 2 shows that after electric treatment the number of thin capillaries
         (with  radius r  < 20 J.tm)  decreases,  while  the number of thick ones  (with  radius
         r  > 20 J.tm)  increases.  Such  reorganization  of the  pore  space  structure  causes
         irreversible increase of the electric conductivity of the specimen by 4 % and of its
         permeability by 105 % a day after the treatment.  In fig.  60, b,  the curves for the
         probability density function for capillaries appear, for specimen of rocks from  the
         second  series  (see  table 9.1).  It is  evident  that a  rock from  the second  series is
         more heterogeneous than one from  the first series.  In this case irreversible change
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