Page 92 - Fundamentals of Reservoir Engineering
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SOME BASIC CONCEPTS IN RESERVOIR ENGINEERING                          31

                     mathematical model to describe the reservoir performance based on insufficient history
                     data can produce erroneous results when used to predict future reservoir performance.

                     If production-pressure history is available it is possible to make an estimate of the GIIP,
                                                                                                   16
                     in a water drive reservoir, using the following method as described by Bruns et.al . The
                     depletion material balance, equ. (1.34), is first solved to determine the apparent gas in
                     place as
                                    G
                           G =        p                                                             (1.42)
                            a
                                 1 −  E /E i
                     If there is an active water drive, the value of G a calculated using this equation, for
                     known values of E and G p, will not be unique. Successive, calculated values of G a will
                     increase as the deviation of p/Z above the depletion material balance line increases,
                     due to the pressure maintenance provided by the aquifer. The correct value of the gas
                     in place, however, can be obtained from equ. (1.40) as

                                G —  W   E
                           G =    p    e                                                            (1.43)
                                  1E /E  i
                                   −
                     where W e is the cumulative water influx calculated, using some form of mathematic
                     aquifer model, at the time at which both E and G p have been measured.




                                                             W  - too small
                                                               e
                                   G a                                     W  - correct model
                                                                             e




                                                                       W  - too large
                                                                         e

                                    G




                                                        W E/ (1−E / E) i
                                                          e

                     Fig. 1.12  Determination of the GIIP in a water drive gas reservoir. The curved, dashed
                                lines result from the choice of an incorrect, time dependent aquifer model;
                                (refer Chapter 9)

                     Subtracting equ. (1.43) from equ. (1.42) gives

                                          WE
                           G =   G +        e                                                       (1.44)
                            a
                                       1 −  E /E i
                     If the calculated values of G a, equ. (1.42), are plotted as a function of W eE/(1−E/E i) the
                     result should be a straight line, provided the correct aquifer model has been selected,
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