Page 253 - Geology and Geochemistry of Oil and Gas
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MODELS OF STATIC GEOLOGIC SYSTEMS                                    219
                If a reservoir is modeled by a bundle of capillary tubes, the rate of flow, q, can be
             given by the Hagen–Poiseuille equation
                         4
                  q ¼ Npr Dp=8mL c                                             (11.16)
                         c
                                               3
             where q is the volumetric flow rate (cm /sec), N is the number of capillaries, r c is the
                                                                                   2
             capillary radius (cm), Dp is the differential pressure across the capillaries (dyn/cm ),
             m is the fluid viscosity (P) and L c is the length of capillaries (cm).
                The Darcy equation for rate of flow q is
                                                                               (11.17)
                  q ¼ kADp=mL c
             where q is the volumetric rate of flow, k is the permeability (darcy), A is the total
                                  2
             cross-sectional area (cm ), Dp is the differential pressure (atm), m is the fluid viscosity
             (cP), and L c is the length of the flow path.
                                                                                    2
                If, instead, viscosity is expressed in poises and differential pressure in dyn/cm ,
             then
                                9
                  q ¼ 9:869   10 kDp=mL c                                      (11.18)
               The porosity f of this bundle of capillary tubes may be expressed as the capillary
             volume V c per unit of bulk volume, V b :
                                                2
                                  2
                  f ¼ V c =V b ¼ Npr L c =AL c ¼ Npr =A                        (11.19)
                                  c             c
               Thus, the total cross-sectional area A of the bundle of capillary tubes is
                          2
                  A ¼ Npr =f                                                   (11.20)
                          c
               The average capillary tube radius r c may be found by combining Eqs. 11.16, 11.17,
             and 11.20:
                  r c ¼ 2ð2k=fÞ 1=2                                            (11.21)
               The surface area per unit of pore volume s p is given by:
                        2         2
                  s p ¼ N pr c L c =Npr L c ¼ 2=r c                            (11.22)
                                  c
               On substituting the value of capillary tube radius from Eq. 11.21 into Eq. 11.22,
             the specific surface area per unit of pore volume, s p , can be expressed as
                            1=2
                  s p ¼ ðf=2kÞ                                                 (11.23)
               For the specific surface area per unit of grain volume of rock consisting of equal-
             size spheres, the following formula was proposed (Buryakovsky et al., 2001):
                                 2                  2          3
                  s g ¼ A=V ¼ Npd ð1   fÞ=V sph ¼ 6Npd ð1   fÞ=Nd p ¼ 6ð1   fÞ=d  (11.24)
             where A is the surface area, V is the bulk volume of rock, V sph is the total volume of
                       3
             spheres (cm ), N is the number of spheres per unit of grain volume, d is the diameter
             of sphere (cm), and f is the porosity (fractional).
                If spheres (grains) are not equal in size, then the specific surface area per unit of
             grain volume of such a rock may be calculated using the following formula:

                                   X
                  s g ¼ ½6ð1   fÞ=100Š  ðC i =d i Þ                            (11.25)
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