Page 222 - Petroleum Geology
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             The macroscopic velocity through the carrier bed is approximately qlf, that
             is, about  160 pm/s,  or  14 m/day.  There  are  no  obvious difficulties in ac-
             cumulating enough  oil  for a  giant  field  in a million years - or even a few
             hundred thousand years.
               The rate of primary migration per unit area of interface between mudstone
             and  carrier bed  is undoubtedly  very slow; but this is probably compensated
             by the very large areas of such interfaces.
               If gas, and gas only, is migrating, the principles are the same except that as
             gas moves to positions of different pressures and temperatures (usually lower)
             its volume changes significantly. If gas and oil are migrating together in separate
             phases, the principles are the same, but the details become very complex be-
             cause gas can dissolve in oil and water. If  oil has gas in solution . . . there are
             many ,variations on the theme. Oil is also slightly soluble in water, so any oil
             left behind in a discontinuous phase will probably be removed eventually in
             solution in moving water.
             Accumulation of petroleum in a trap


               When petroleum, trickling along one or more paths of local minimum poten-
             tial, arrives in the trap and begins to accumulate,  migration  ends but a new
             set of  physical changes begins:
               -Water  is displaced downwards from the top of the reservoir.
               - The oil/water or gaslwater contact is displaced downwards.
               - The pressure in the petroleum increases while petroleum accumulates.
               -The  petroleum  in  the  accumulation  continues to move in response to
             these changes.
               Migrating  petroleum  has  negligible  kinetic  energy, so  the  newly-arrived
             petroleum is added to the accumulation at the interface, without penetration
             into the accumulation (much as cream poured  into a jug, rather than milk).
             The  water  contact will be rather lower near the point  of  entry. Due to the
             density  difference  between  oil  and water, and gas and water, the potential
             energy of  the accumulation  will be greater where the water contact is lower,
             and there will be sympathetic movement within the accumulation in the direc-
             tion that tends to restore equilibrium.
               Within  the accumulation, a  new  physical  environment  develops.  Within
             the continuous oil phase, the pressure decreases with elevation above the oil/
             water contact according to the relationship:
                                                                              (9.10)
            This rate of  decrease is less than that in a continuous water phase, so that, if
            we  take  their  pressures to be equal at the oil/water contact, the oil at any
            depth within the reservoir above this is at a higher pressure than the water in
            continous phase with it. This greater pressure is applied to the water, which
            acquires the pressure  gradient  Ap,/Az   = pog, and  so  acquires a downward
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