Page 180 - Fundamentals of Reservoir Engineering
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DARCY'S LAW AND APPLICATIONS                               118

                     and results from defining k in equ. (4.8) as the permeability, rather than the K in
                     equ. (4.3), the latter having a dependence on the fluid properties. The permeability so
                     defined is termed the absolute permeability.

                     If there are two fluids, such as oil and water, flowing simultaneously through a porous
                     medium, then each fluid has its own, so-called, effective permeability. These
                     permeabilities are dependent on the saturations of each fluid and the sum of the
                     effective permeabilities is always less than the absolute permeability. The saturation
                     dependence of the effective permeabilities of oil and water is illustrated in fig. 4.8(a). It
                     is conventional to plot both permeabilities as functions of the water saturation alone
                     since the oil saturation is related to the former by the simple relationship S o = 1−S w.

                     Considering the effective permeability curve for water, two points on this curve are
                     known. When S w = S wc, the connate or irreducible water saturation, the water will not
                     flow and k w = 0. Also, when S w = 1 the rock is entirely saturated with water and k w = k,
                     the absolute permeability. Similarly for the oil, when S w = 0 (S o = 1) then k o = k and,
                     when the oil saturation decreases to S or, the residual saturation, there will be no oil flow
                     and k o = 0. In between these limiting values, for both curves, the effective permeability
                     functions assume the typical shapes shown in fig. 4.8(a). The main influence on the
                     shapes of the curves appears to be the wettability, that is, which fluid preferentially
                                               8
                     adheres to the rock surface . Although it is difficult to quantify this influence, the
                     permeability curves can be measured in laboratory experiments for the wettability
                                                        9
                     conditions prevailing in the reservoir .
                                      absolute
                      k              permeability          k     1                                   1


                                                                            k′ ro




                      k o                                  k w
                                                                                          k′ rw       k rw








                      0 0                                  0     0 0                                 0
                        0      S wc     S w      1-S or   1       0     S wc       S w      1-S or  1


                     Fig. 4.8   (a) Effective and (b) corresponding relative permeabilities, as functions of the
                                water saturation. The curves are appropriate for the description of the
                                simultaneous flow of oil and water through a porous medium

                     The effective permeability plots can be normalised by dividing the scales by the value
                     of the absolute permeability k to produce the relative permeabilities

                                    k(S )                k(S )
                           k(S ) =   o  w  and k (S ) =   w   w                                     (4.30)
                            ro
                                w
                                      k          rw  w      k
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