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MIGRATION AND ACCUMULATION OF PETROLEUM                  51



                            at a temperature of  about 200°F.  This temperature is well within the
                            temperature range for generation of  petroleum and thus may assist in
                            the primary migration of  oil when smectites are present in the shale
                            body [6].

                     SECONDARY MIGRATION


                              Inasmuch as petroleum reservoirs exist in a water environment, the
                            migration  of  hydrocarbons  from  the  point  of  release  from  a  source
                            rock  to  the  top  of  the  trap  is  intimately  associated  with  capillary
                            pressure  phenomena  and  hydrology.  The  pore  size  distributions,
                            tortuosity of continuous channels, porosity, permeability, and chemical
                            characteristics of reservoir rocks and their interstitial fluids differ widely.
                            Nevertheless, because of  the ubiquitous presence of water, capillarity,
                            buoyancy, and hydrology apply in all cases [ 141.
                              The  migration of  oil as  distinct droplets in water-saturated rock  is
                            opposed by the capillary forces, which are functionally related to pore
                            size, interfacial tension between oil and water, and adhesion of  oil to
                            mineral surfaces (wettability).  This is expressed through a contact angle
                            for a capillary of uniform size as:





                            where:  P,  = capillary pressure, Pa.
                                    o  = interfacial tension, (NX  10-3)/m.
                                    8  = contact angle.
                                    r,  = radius of the capillary, m.

                              The  more usual case is  one in which  the oil droplet exists within
                            the confines of a large pore containing several smaller-sized pore throat
                            exits (Figure  2.9).  Under  these  conditions, the  pressure required  to
                            displace the droplet from the large pore  through the constriction of
                            a pore  throat (the  displacement pressure)  is  the  difference between
                            the capillary pressures of the leading (l) and trailing (t) pores [61:


                                                                                           (2.5)


                            where:  Pd  = displacement pressure, Pa.
                                    61 = contact angle of the leading edge.
                                    et  = contact angle of the trailing edge.
                                    rl  = radius of the leading pore, m.
                                    rt  = radius of the trailing pore, m.
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