Page 66 - Fundamentals of Reservoir Engineering
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SOME BASIC CONCEPTS IN RESERVOIR ENGINEERING                           5

                     −    osmosis between waters having different salinity, the sealing shale acting as the
                          semi-permeable membrane in this ionic exchange; if the water within the seal is
                          more saline than the surrounding water the osmosis will cause an abnormally
                          high pressure and vice versa.

                     Some of these causes of abnormal pressuring are interactive, for instance, if a
                     reservoir block is uplifted the resulting overpressure is partially alleviated by a decrease
                     in reservoir temperature.

                                                         3
                     The geological textbook of Chapman provides a comprehensive description of the
                     mechanics of overpressuring. Reservoir engineers, however, tend to be more
                     pragmatic about the subject of abnormal pressures than geologists, the main questions
                     being; are the water bearing sands abnormally pressured and if so, what effect does
                     this have on the extent of any hydrocarbon accumulations?

                     So far only hydrostatic pressures have been considered. Hydrocarbon pressure
                     regimes are different in that the densities of oil and gas are less than that of water and
                     consequently, the pressure gradients are smaller, typical figures being

                              dp
                                    =  0.45 psi/ ft
                              dD   water


                              dp
                                     =  0.35 psi/ ft
                             dD  oil

                              dp
                                     =  0.08 psi/ ft
                              dD   gas

                     Thus for the reservoir containing both oil and a free gascap, shown in fig. 1.3; using the
                     above gradients would give the pressure distribution shown on the left hand side of the
                     diagram.

                     At the oil-water contact, at 5500 ft, the pressure in the oil and water must be equal
                     otherwise a static interface would not exist. The pressure in the water can be
                     determined using equ. (1.5), rounded off to the nearest psi, as
                           p w  =  0.45 D +  15 (psia)                                               (1.7)
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