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190           CHAPTER 11  GAS COLMATATION IN ELECTRIC ACTION

            The equations (11.31),  (11.32)  are good for  describing the growth of a single
         bubble in a boundless medium.  However there may be many bubbles in a capillary
         and the average distance between them may be relatively small compared to their
         size (la  ~ (10 -10 3 )a).  Therefore it is necessary to take into account the interaction
         of thermal fields of the bubbles.
            Suppose that at the time dt, an amount of energy equal to 7rr 2 le(t) was released
         in a capillary.  (In the general case, heat losses caused by the outflow through the
         capillary surface must  be taken into account in e(t).)  Furthermore, suppose that
         this  amount  of energy  was  distributed  uniformly  among 7rr 2 ln0  bubbles  in  the
         capillary.  Now, taking into account QJ  ~ qp, we obtain
                                                                           (11.34)

            If we  assume  that  not  all,  but  only  a  part  of the  energy  e(t)  was  used  for
         supplying heat to the bubbles, then the rest of the energy will be used for the fluid
         overheating.  The latter will make heat losses through the capillary surface larger,
         and therefore will decrease e(t).  In its turn, this will create an additional flow q/

         in (11.28), which is going to partially comensate the mentioned loss, and therefore
         is  likely  to make  the quantity QJ  closer  to  e(t)fn0  in  its value.  It is  possible to
         estimate the additional flow  qf, which may cause deviation from  equality (11.34),
         as follows.  If there is no heat discharge, the temperature at a distance ""' la  from
         a  bubble  must  grow  by  approximately  AT =  e(t)rk/(Cfpf)  in  a  characteristic
         period of temperature equalizing

                                        Tk = l~/Kt

         Therefore q/  ~ kJATl; 1 47ra 2  ~ 10a 2 lae(t).
            In this case the ratio
                                                                           (11.35)
         since (afla) « 1.
            Initial conditions

                               a(O) = ao,  Pp(O) =PI+ 2xfao
         and  the equations  (11.27),  (11.26),  (11.31),  (11.33),  (11.34)  define  the relations
         a(t) and Pp(t)  completely.
            Introduce the notations

                   Ao  = no(4/3)7rag,  A= Ao(no/n.),  X= Qp/(PJLp),
                                                 1
                                  H = XoRpTpPJP~ ,   Z = 2xf(aopoo)
         and the dimensionless variables

                            O.  =  Xt,  w. =  afao,  G. = Pp/Poo
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