Page 186 - Principles of Applied Reservoir Simulation 2E
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Part II: Reservoir Simulation  171


             Peaceman  showed that the shut in pressure P ws of an actual well equals
        the simulator well block pressure P 0 at a shut in time A/ 5 given by

                                                                     (17.1)
                                f
                                         K
        where K is permeability,  <f) is porosity, |l is viscosity, and C T is total compress-
        ibility. Units for all variables are given in Table 17-2 at the end of this section,













                                                   Log  (T;, +  AO/A/

              Figure  17-2.  Horner plot of PBU.

             The relationship between gridblock pressure P 0 and flowing pressure  P wf
        at the wellbore is


                     P..., = P.  -  141.2    In  —  +  S             (17,2)
                                                 r.

        where Q is the flow rate, B is formation  volume factor, and S is skin. For an
        isotropic reservoir, that is, a reservoir in which x-direction permeability equals
                                = K y),  the equivalent well block radius is given in
        y direction permeability (K x
        terms of the block lengths  {A*, Ay}, thus
                                        2      2 /2
                             =  0.14  (A*  +  A>> )'                 (17.3)
                          r o
        shut  in time can  be  masked  by  wellbore  storage  effects.  If  it  is,  the  shut in
        pressure P^  may have to be obtained by extrapolation of another part of the
        curve, such  as the  radial  flow  curve.  Table  17-2  summarizes  the  parameters
        involved in the Peaceman correction for a consistent set of units. An application
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