Page 473 - Petrophysics
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RADIAL FLOW SYSTEMS           44 1


                           Equation 7.68 can be written in oilfield units as follows:
                                           kh  ]
                                    1  l4l.2qs,pB
                                    4
                           Pi-@=-[                                                      (7.69)
                           The right-hand side of this equation corresponds to the amount of fluid
                           produced, causing the reservoir pressure to drop from pi  to p. It can be
                           demonstrated that this pressure drop is also expressed as:


                                                                                        (7.70)


                           If Equations 7.69 and 7.70 are combined, one obtains for time t:


                                                                                        (7.71)


                           where t is in hours, ct is the total compressibility in psi-’  and the permea-
                           bility is in mD. Craft and Hawkins defined this time as the readjustment
                           time, tr, or the time required to establish a logarithmic pressure distri-
                           bution between r,  and re 111.  For a well in a fully active water drive
                           reservoir,  i.e.,  f  = 1,  the  constant 0.25 in  Equation  7.69 is  replaced
                           by  0.50, and the constant 474.5 in Equation 7.71 is replaced by  949.
                           Generally, steady-state flow equations should be used only when t,  is
                           small compared to the total producing life of the reservoir. If tr is too large,
                           as it is often the case in fully active water-drive reservoirs, unsteady-state
                           flow equations must be used.


                             Skin Zone
                             In many cases, it has been found that the permeability in the vicinity
                           of  the wellbore differs from that in the major portion of  the reservoir
                           as shown in Figure 7.7. This zone of altered permeability, ks, and radial
                           extent, rs, is called the “skin,” and the degree of alteration is expressed in
                           terms of the skin factor s [23, 241. The permeability of the skin zone can
                           be reduced (s > 0) as a result of  drilling and well completion practices
                           as discussed in the next chapter.
                             The  average  permeability  of  the  formation  in  the  vicinity  of  the
                           wellbore  also  can  be  higher  (s  < 0)  than  that  in  the  major  portion
                           of  the  reservoir  after fracturing or  acidizing the  well  at  completion.
                           Therefore, all the radial flow rate equations in this section, which were
                           derived on the basis that the permeability of  the formation is the same
                           between r,  and re, must be modified to include the effect of  skin. This
                           can be done either by subtracting the additional pressure drop (due to
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