Page 88 - Fundamentals of Reservoir Engineering
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SOME BASIC CONCEPTS IN RESERVOIR ENGINEERING                          27

                                                 GS
                           V w  =  PV ×  S wc  =    wc
                                              E(1 S )
                                                  −
                                                     wc
                                                i
                     the reduction in hydrocarbon pore volume, equ. (1.38), can be included in equ. (1.33),
                     to give

                           G p            (c S wc  + c ) p    E                                     (1.39)
                                                      ∆
                                            w
                                                    f
                           G   =  1−   1 −    1 S wc          E i
                                               −

                                                                                             −6
                     as the modified material balance. Inserting the typical values of c w = 3 × 10 /psi,
                                −6
                     c f = 10 × 10 /psi and S wc = 0.2 in this equation, and considering a large pressure drop
                     of ∆p = 1000 psi; the term in parenthesis becomes
                               (3 .2 10)       6     3
                                  ×
                                     +
                                               −
                           1 −             × 10 × 10 =   1 0.013
                                                          −
                                   0.8
                     That is, the inclusion of the term accounting for the reduction in the hydrocarbon pore
                     volume, due to the connate water expansion and pore volume reduction, only alters the
                     material balance by 1.3% and is therefore frequently neglected. The reason for its
                     omission is because the water and pore compressibilities are usually, although not
                     always, insignificant in comparison to the gas compressibility, the latter being defined in
                     sec. 1.6 as approximately the reciprocal of the pressure. As described in Chapter 3,
                     sec. 8, however, pore compressibility can sometimes be very large in shallow
                                                                              −6
                     unconsolidated reservoirs and values in excess of 100 × 10 / psi have been
                     measured, for instance, in the Bolivar Coast fields in Venezuela. In such reservoirs it
                     would be inadmissible to omit the pore compressibility from the gas material balance.
                     In a reservoir which contains only liquid oil, with no free gas, allowance for the connate
                     water and pore compressibility effects must be included in the material balance since
                     these compressibilities have the same order of magnitude as the liquid oil itself (refer
                     Chapter 3, sec. 5).

                     In the majority of cases the material balance for a depletion type gas reservoir can
                     adequately be described using equ. (1.35). This equation indicates that there is a linear
                     relationship between p/Z and the fractional recovery G p/G, or the cumulative production
                     G p, as shown in fig. 1.10(a) and (b), respectively. These diagrams illustrate one of the
                     basic techniques in reservoir engineering which is, to try to reduce any equation, no
                     matter how complex, to the equation of a straight line; for the simple reason that linear
                     functions can be readily extrapolated, whereas non-linear functions, in general, cannot.
                     Thus a plot of p versus G p/G or G p, would have less utility than the representations
                     shown in fig. 1.10, since both would be non-linear.
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