Page 218 - Fundamentals of Reservoir Engineering
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OILWELL TESTING                                    156

                     The constant terminal rate solution of the radial diffusivity equation during the late
                     transient flow period is too complicated to include at this stage. A simplified method of
                     obtaining this solution will be described in sec. 7.6.

                     Once semi-steady state conditions prevail the solution can be determined by adding
                     the simple material balance equation for the bounded drainage volume

                                 p −
                           cAhφ ( i    ) p =  qt                                                    (7.12)

                     to the semi-steady state inflow equation

                                      qµ            4A
                           pp  wf  =  2kh       ½ ln  γ C r 2  +  S                                 (6.22)
                             −
                                      π
                                                     Aw
                     to give

                                     qµ             4A            kt
                           p wf  =  p −  2kh      ½ ln  γ Cr 2  +  2π  φ µ cA  +  S                 (7.13)
                                 i
                                     π
                                                     Aw

                     In this equation p is the current average pressure within the drainage boundary and C A
                     is the Dietz shape factor introduced in Chapter 6, sec.5. The magnitude of C A depends
                     on the shape of the area being drained and also upon the position of the well with
                     respect to the boundary.

                     Theoretically, for the constant terminal rate solution, the rate q in equs. (7.12) and
                     (6.22) is the same. In practice, it is sometimes difficult to maintain the production rate of
                     a well constant over a long period of time and therefore, the current rate in equ. (6.22)
                     may differ from the average rate which is implicitly used in material balance, equ.
                     (7.12). In this case the rate in equ. (7.12) is set equal to the current, or final flow rate,
                     and the flowing time is expressed as an effective flowing time, where

                                                        Cumulative Production
                           t  =  Effective flowing time  =                                          (7.14)
                                                              Final flow rate

                     Use of the effective flowing time is therefore simply a method for equalising the rates
                     and preserving the material balance and is frequently used in pressure analysis, as will
                     be described later.

                     Even though no equation for describing the pressure decline during the late transient
                     flow period has yet been developed, equs. (7.10) and (7.13), which are appropriate for
                     transient and semi-steady state flow, can be usefully employed by themselves in well
                     test analysis.

                     Well testing involves producing a well at a constant rate or series of rates, some of
                     which may be zero (well closed in), while simultaneously taking a continuous recording
                     of the changing pressure in the wellbore using some form of pressure recording device.
                     The retrieved record of wellbore pressure as a function of time can be analysed in
                     conjunction with the known rate sequence to determine some or all of the following
                     reservoir parameters:
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