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RADIAL DIFFERENTIAL EQUATION FOR FLUID FLOW                         135

                     since it was assumed in deriving equ. (5.1) that the porous medium was completely
                     saturated with a single fluid thus implying the use of the absolute porosity.
                     Alternatively, allowing for the presence of a connate water saturation, the φc product
                     can be interpreted as

                                               (c S + c S    +  c )
                           φ  absol ute  (1 − S wc) ×   o  o  w  wc  f                              (5.24)
                                                    (1 S )
                                                      −
                                                          wc
                     in which φ absolute  (1 − S wc) is the effective, hydrocarbon porosity, and the
                     compressibility is equivalent to that derived in Chapter 3, equ. (3.19), which is used in
                     conjunction with the hydrocarbon pore volume. In either event, the products expressed
                     in equs. (5.23) and (5.24) have the same value, the reader must only be careful not to
                     mix the individual terms appearing in the separate equations.

                     Equation (5.20) is the radial diffusivity equation in which the coefficient k/φµc is called
                     the diffusivity constant. This is an equation which is frequently applied in physics, for
                     instance, the temperature distribution due to the conduction of heat in radial symmetry
                     would be described by the equation

                           1 ∂    ∂ T    1 T
                                         ∂
                                 r     =
                           rr ∂    r ∂    K t ∂

                     in which T is the absolute temperature and K the thermal diffusivity constant. Because
                     of the general nature of equ. (5.20) it is not surprising that many reservoir engineering
                     papers, when dealing with complex solutions of the diffusivity equation, make reference
                                                                                               3
                     to a text book entitled "Conduction of Heat in Solids", by Carslaw and Jaeger , which
                     gives the solutions of the equation for a large variety of boundary and initial conditions
                     and is regarded as a standard text in reservoir engineering.


                     REFERENCES

                     1)    Matthews, C.S., Brons, F. and Hazebroek, P., 1954. A Method for Determination
                           of Average Pressure in a Bounded Reservoir. Trans. AlME. 201: 182-191.

                     2)    Dranchuk, P.M. and Quon, D., 1967. Analysis of the Darcy Continuity Equation.
                           Producers Monthly, October: 25-28.

                     3)    Carslaw, H.S. and Jaeger, J.C., 1959. Conduction of Heat in Solids. Oxford at the
                           Clarendon Press, (2nd edition).
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