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OILWELL TESTING                                    189

              7.7    PRESSURE BUILDUP ANALYSIS TECHNIQUES

                     The remaining sections of this chapter concentrate on the practical application of the
                     theory developed so far to the analysis of well tests. It is considered worthwhile at this
                     stage to change from Darcy to field units since, in practice, tests are invariably
                     analysed using the latter and the majority of the literature on the subject employs these
                     units. All equations in the remainder of this chapter will therefore be formulated using
                     the field units specified in table 4.1. Since a great many of the equations are expressed
                     in dimensionless parameters they remain invariant, or at least partially invariant in
                     form. For instance, the most significant equation in the present subject of pressure
                     buildup analysis is that describing the theoretical linear buildup, which in Darcy units, is

                           2kh                       t +∆ t              4t D
                            π
                                                               t
                                                                  −
                                              =
                                   p −
                                                                D
                                  ( i  p ws(LIN) ) ½ ln   + p D  () ½ ln                            (7.37)
                            q µ                        t ∆               γ
                     and which, on conversion to field units becomes
                                      kh                         t +∆ t              4t
                           7.08 10 -3      (p − p    ) 1.151 log      + p  () −  ½ ln  D            (7.48)
                                                                           t
                                                      =
                                ×
                                     qB  o   i   ws(LIN)            t ∆  D  D         γ
                                      µ
                     The conversion of the left hand side of this equation has already been described in
                     exercise 7.3 and is necessary to preserve this expression as dimensionless, in field
                     units. The only change to the right hand side is that the natural log of the
                     dimensionless time ratio has been replaced by log 10, which is mainly required for

                     plotting purposes, the remainder of the equation is invariant in form. Thus the p D
                     function is still

                                                 4t
                                     π
                           p(t ) =  2   t DA  + ½ ln  D  − ½ p D(MBH)  (t )                         (7.42)
                               D
                            D
                                                                DA
                                                 γ
                     which is totally invariant, although in evaluating this expression it must be remembered
                     that now
                                           kt
                           t =  0.000264      2  (t-hours)                                          (7.20)
                            D
                                         φµ cr w

                     and

                                            kt
                           t DA  =  0.000264     (t-hours)                                          (7.49)
                                          φµ cA

                     The p D(MBH) term is, in the majority of cases, just a number read from the MBH charts
                     corresponding to t DA evaluated in field units. Only when used to calculate p using the
                     MBH method does it require interpreting as

                                              kh
                           p D(MDH)  =  0.01416    ( p * p )
                                                       −
                                             qB  o
                                              µ
                     The Horner plot for a typical buildup is shown as fig. 7.18.
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