Page 179 - Percolation Models for Transport in Porous Media With
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176          CHAPTER 10  PRODUCTION CHANGE: ELECTRIC ACTION

         of w;/(E"Qo) are presented, and 1/J;(L")  are presented in fig.  66,  b.
            It is  clear from  these plots that w; /  (  E"  Qo)  decreases and 1/Je  increases as F"
         grows and  L" diminishes.  These dependencies are more sensitive to the changes
         in the quantity L" than they are to the changes in  F".  The value Q/Qo depends
         weakly on the parameters of the problem and varies from  1.5 to 2.5.
            Two regions are shown  in  fig.  67 in  the plane of the parameters F"  and  L".
         The boundaries of those  regions,  where  the optimal electric treatment regime is
         possible,  form  region  I.  The  boundaries of those  regions,  where  the maximum
         of 1/Je  does  not exist, and consequently the treatment regime with small currents
         (we  <we) is optimal as far  as  the energy consumption costs are concerned, form
         region II.
            Therefore depending on  the values of the parameters L" and  F"  determined
         from  the plot of K(T), both the presence and the absence of an extremum of the
         function  1/Je  are possible.  In  principle,  the optimal electric treatment regime can
         be determined based on  the calculated data (see figs.  65  - 67)  and  the economic
         calculations.  For an arbitrary form  of the K(T) dependence,  the optimal electric
         treatment regime is determined similarly from the solution to the equation (10.28).
         Note that even when the electric treatment is carried out in  non-optimal regimes,
         the economic effect is positive.  This is due to the fact that the time of maintenance
         of  the  wells,  necessary  for  the  development  of a  deposit  (i.e.,  for  reaching  the
         established level of the recovery of the useful component), is  made less.


         10.3  Results of Field Studies


         Typical  diagrams  of electric  energy  supply  to  the  reservoir,  which  have  already
         been  tested, are presented in  fig.  63 for  the case of a single well.  In diagram I I I
         voltage is supplied from  the source directly to the casing column.  In this case it
         is  not  necessary  to immerse  an  electrode  into  the  well.  This  diagram  is  rather
         simple and efficient,  but if the reservoir lies  more than 300 meters deep,  then the
         electric energy consumption due to the current flow through the lateral area of the
         wells becomes very large.  In this case it is advisable to use a different diagram of
         energy supply.  Experimental work  done with  objects of various geological  types
         in  different  regions  (over  80  places)  showed  that  the  well  production  rates  can
         increase by 2 to 20 times (at an average of 1.5 to 2 times) after electric treatment.
            Experiments showed  that  well  production  rates  keep  stable for  two  to  three
         years after the electric treatment.  A positive effect  is  observed for  electric treat-
         ment of different  types of rocks,  e.g.  sandy-argillaceous, carbonate, or fractured
         ones.  The studies involving observation wells showed that the changes of perme-
         ability after the electric treatment are registered at distances up to 10m (fig.  68).
         A typical correlation for the modification of a hydrogeological well production rate
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