Page 206 - Fundamentals of Reservoir Engineering
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STABILIZED INFLOW EQUATIONS                                144

                                    2k h
                                     π
                           PI =         e
                                    r   1
                               µ   ln  e  −  +  S
                                    r w  2

                     the Pl ratio increase is

                                660   1
                             ln     −   +  254.02  261.11
                           =   .333   2 1        =
                                 660
                               ln     −  −  3.09    4.00
                                 .333  2
                           =  65.3


              6.5    GENERALIZED FORM OF INFLOW EQUATION UNDER SEMI-STEADY STATE
                     CONDITIONS

                     The semi-steady state inflow equation developed in sec. 6.2 appears to be restrictive in
                     that it only applies for a well producing from the centre of a circular shaped drainage
                     area. When a reservoir is producing under semi-steady state conditions each well will
                     assume its own fixed drainage boundary, as shown in fig. 5.3, and the shapes of these
                     may be far from circular. The inflow equation will therefore require some modification to
                     account for this lack of symmetry. Equation (6.12) can be expressed in a generalized
                                                                        3
                     form by introducing the so-called Dietz shape factors denoted by C A, which are
                     presented for a variety of different geometrical configurations in fig. 6.4. Precisely how
                     these shape factors were generated, in the first place, will be explained in the
                     appropriate place, Chapter 7, sec. 6. For the moment the reader is asked to accept the
                     following tenuous argument for the generalization of the inflow equation. Excluding the
                     mechanical skin factor, equ. (6.12) can be expressed as

                                     qµ   1      r π  2
                           pp  wf  =  2kh 2 ln π r e e 3/ 2                                         (6.20)

                             −
                                                2
                                     π


                                                w
                     in which the argument of the natural log can be modified as
                             4r e 2     4A        4A                                                (6.21)
                              π
                               3/2 2
                           4 e r  w  =  56.32r w 2  =  γ 31.6r w 2
                            π
                     in which A is the area being drained, γ is the exponential of Euler's constant and is
                     equal to 1.781, and 31.6 is the Dietz shape factor for a well at the centre of a circle,
                     refer fig. 6.4. Therefore, equ. (6.20) can be expressed in the general form, including the
                     skin factor, as

                                     qµ   1    4A
                           pp  wf  =  2kh 2 ln γ C r 2  + S                                         (6.22)

                             −
                                     π

                                                Aw
                     For a reservoir which is producing under semi-steady state conditions, then as already
                     noted, the volume drained by each well is directly proportional to the well's production
                     rate. Therefore, it is a fairly straightforward matter to estimate the volume being drained
                     by each well and, using the average thickness in the vicinity of the well, the area. If
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