Page 214 - Petroleum Geology
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              PO           P
                   h,  =  ___   h  -2.                                          (9.5)
            P  -Po       P -Po
            Thus, if  there is enough data to map h and z, we can map h,.  We  shall return
            to this equation.
              Clearly, the projection of the direction of water movement on a horizontal
            surface is the same as that for oil movement ,while the oil is migrating with-
            out constraint from the cap rock.  Both oil and water equipotential surfaces
            are  inclined  in the direction of  water motion, but by different amounts.  If
            the water  flow is directly downdip, there is some critical dip that equals the
            “dip” of the oil equipotential surfaces and is normal to the migration path of
            the oil through the water. A small volume of oil under a cap rock at this critical
            dip would not move.
              Huljbert  (1953,  pp.  1986-1987)  has  shown  that  this  critical dip, Be,  is
            given by:

                       P    dh
            tan6,  =   ~    -
                    P-Po    dx
            where dh/dx is the slope of the water’s potentiometric  surface as given, for
            example, by the contour interval divided by the distance separating two con-
            tours on the potentiometric surface (not the hydraulic gradient, in which the
            length  is  measured  along  the aquifer). The coefficient p /(p - p o) indicates
            that  the heavier the oil, the steeper the slope of  the oil’s equipotential sur-
            faces and the critical dip. If  the oil’s density equals that of the water, oil can
            only accumulate by capillary effects because there is no gravitational effect
            that will accumulate it.
              Gas has a more nearly vertical migration path across a carrier bed by virtue
            of  its  smaller density  relative  to  oil  and water.  The consequences of  these
            effects separately on oil and on gas may well not be the same as the combined
            effect. If  gas alone would take the path G in Fig. 9-7, and oil alone the path
            0, it is most  unlikely that these would  be the paths if  both were migrating
            simultaneously. Some intermediate path depending on saturations would be
            more likely.
              Once restrained by the upper surface of the carrier bed, further migration
            follows paths  of  local  minimum  potential.  These will not in general be in-
            dicated by a detailed contour map of the interface between the cap rock and
            the carrier bed; but if  the contours were drawn relative, not to sea level but
            to a surface at the critical dip, such a map would indicate the possible paths
            of  migration.
              To get an idea of  the magnitudes of  the critical dip or slope 6,,   consider
            a potentiometric  surface  with  a  slope of   which is about the steepest
            regional  slope of  the Great  Artesian  basin  of  Australia.  This  is a  slope of
            about  3  min  of  arc.  The mass density of  most  crude oils falls in the range
            750400 kg m- 3,  so the amplifying factor ranges from four to ten, and the
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