Page 90 - Fundamentals of Reservoir Engineering
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SOME BASIC CONCEPTS IN RESERVOIR ENGINEERING                          29

                     can be checked against the volumetric estimate obtained as described in secs. 1.2 and
                     1.3. This technique of matching the observed production pressure history by building a
                     suitable mathematical model, albeit in this case a very simple one, equ. (1.35), and
                     using the model to predict future performance is one which is fundamental to the
                     subject of Reservoir Engineering.

                     b)   Water drive reservoirs

                     If the reduction in reservoir pressure leads to an expansion of the adjacent aquifer
                     water, and consequent influx into the reservoir, the material balance equation must
                     then be modified as

                           Production   =  GIIP −   Unproduced Gas
                              (sc)         (sc)          (sc)                                       (1.40)
                                                         G
                              G p       =  G     −        − W E
                                                             e
                                                        E i

                     where, in this case, the hydrocarbon pore volume at the lower pressure is reduced by
                     the amount W e, which is the cumulative amount of water influx resulting from the
                     pressure drop. The equation assumes that there is no difference between surface and
                     reservoir volumes of water and again neglects the effects of connate water expansion
                     and pore volume reduction.

                     If some of the water influx has been produced it can be accounted for by subtracting
                     this volume, W p, from the influx, W e, on the right hand side of the equation. With some
                     slight algebraic manipulation equ. (1.40) can be expressed as

                           p   p     G  p        WE
                                                     i
                                                   e
                             =  i    1−        1−                                                   (1.41)
                           Z   Z i    G            G
                     where W e E i /G represents the fraction of the initial hydrocarbon pore volume flooded
                     by water and is, therefore, always less than unity. When compared to the depletion
                     material balance, equ. (1.35), it can be seen that the effect of the water influx is to
                     maintain the reservoir pressure at a higher level for a given cumulative gas production.
                     In addition, equ. (1.41) is non-linear, unlike equ. (1.35), which complicates both history
                     matching and prediction. Typical plots of this equation, for different aquifer strengths,
                     are shown in fig. 1.11.

                     During the history matching phase, a separate part of the mathematical model must be
                     designed to calculate the cumulative water influx corresponding to a given total
                     pressure drop in the reservoir; this part of the history match being described as "aquifer
                     fitting". For an aquifer whose dimensions are of the same order of magnitude as the
                     reservoir itself the following simple model can be used
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