Page 154 - Fundamentals of Reservoir Engineering
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MATERIAL BALANCE APPLIED TO OIL RESERVOIRS                          93

                                            2
                                               2
                           W =  (c +  c ) (r −  r )fhφ ∆ p                                          (3.27)
                                        π
                             e
                                       f
                                           e
                                               o
                                  w
                     in which r e and r o are the radii of the aquifer and reservoir, respectively, and f is the
                     fractional encroachment angle which is either Θ/2π or Θ/360°, depending on whether Θ
                     is expressed in radians or degrees. It should be realised that the only term in
                     equ. (3.27) which is known with any degree of certainty is π! The remaining terms all
                     carry a high degree of uncertainty. For instance, what is the correct value of r e? Is the
                     aquifer continuous for 20 kilometers or is it truncated by faulting? What is the correct
                     value of h, the average thickness of the aquifer or φ, the porosity? These can only be
                     estimated, based on the values determined in the oil reservoir. For such reasons,
                     building a correct aquifer model to match the production and pressure data of the
                     reservoir is always done on a "try it and see" basis and even when a satisfactory model
                     has been achieved it is seldom if ever, unique. Therefore, the most appropriate way of
                     applying equ. (3.26) is by expressing it as

                           F        W
                              =  N +  e                                                             (3.28)
                           E o      E o


                     and plotting F/E o, corresponding to the observed production, versus W e/E o, where We
                     is calculated using an aquifer model such as equ. (3.27).

                                                           w  - too small
                                                             e
                                                                         w  - correct
                                                                           e
                                                                             incorrect geometry
                                  F
                                                                             w  - too large
                                  E o                                          e
                                (stb)



                                              45°

                                           N



                                                           w / E  (stb)
                                                            e
                                                               o
                     Fig. 3.9   Trial and error method of determining the correct aquifer model
                                (Havlena and Odeh)

                     This model is linked to the reservoir by the pressure drop term ∆p which is interpreted
                     as the pressure drop at the original reservoir-aquifer boundary, and is normally
                     assumed to be equal to the average pressure drop in the reservoir due to the
                     production of fluids. If the aquifer model is incorrect, the plotted data points will deviate
                     from the theoretical straight line which has a slope of 45° and intercept N, when
                     W e/E o = 0, as shown in fig. 3.9.

                     The deviation labelled as being due to using the wrong geometry means that radial
                     geometry has been assumed whereas linear geometry would probably be more
                     appropriate. With radial geometry there is a larger body of water in close proximity to
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