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MATERIAL BALANCE APPLIED TO OIL RESERVOIRS                          98

                     Compaction, and its associated effect of surface subsidence, will be much more
                     pronounced for shallow, unconsolidated reservoirs than for the deeper, more
                     competent sands. It is therefore necessary to experimentally determine the
                     compressibility of shallow reservoir sands in order to estimate to what degree
                     compaction will enhance the hydrocarbon recovery, and also, to enable the prediction
                     of the resulting surface subsidence, which can cause serious problems if the surface
                                                                      13
                     location of the field is adjacent to the sea or a lake .

                     Unfortunately, the deformation of unconsolidated sands is usually inelastic and this in
                     turn leads to complications in relating laboratory measured compressibilities to the in-
                     situ values in the reservoir. The nature of the problem can be appreciated by referring
                     again to fig. 3.12. Suppose that both the grain and fluid pressures in a reservoir are
                     normal so that under initial conditions the reservoir is at point B on the compaction
                     curve. The process of cutting a core and raising it to the surface will cause unloading,
                     which for a rock which deforms inelastically, will place the core at point C′, which lies
                     off the normal compaction curve. During the re-loading the horizontal path B−C′ is not
                     reversed, instead there is a mechanical hysteresis effect which means that the true
                     compaction curve is not re-joined until point D, where p D > p B. As a result, the
                     laboratory measured compressibility, determined as the slope of the line C′−D at
                     pressure p B, will be somewhat lower than the in-situ value, which is the slope of the
                     normal curve at p B. Thus, initial values of the in-situ compressibility are difficult to
                     determine and usually require estimation by back extrapolation of laboratory values
                     obtained for grain pressures in excess of p D.

                     The above description of the various complications in estimating in-situ, uniaxial
                     compressibility has been applied for the extreme case of a perfectly inelastic reservoir
                     rock. Generally rock samples are neither perfectly elastic or inelastic but somewhere in
                     between. Nevertheless, the same qualitative arguments apply and it is therefore not
                     always meaningful to merely estimate in-situ compressibilities by reference to
                     published charts for typical sandstones and limestones.

                     REFERENCES


                     1)    Schilthuis, R.J., 1936. Active Oil and Reservoir Energy. Trans.,
                           AIME, 118: 33-52.


                     2)    Amyx, J.W., Bass, D.M., and Whiting, R.L., 1960. Petroleum Reservoir
                           Engineering - Physical Properties. McGraw-Hill: 448-472.

                     3)    McCain, W.D., 1973. The Properties of Petroleum Fluids. Petroleum Publishing
                           Company, Tulsa: 268-305.

                     4)    Havlena, D. and Odeh, A.S., 1963. The Material Balance as an Equation of a
                           Straight Line. J.Pet.Tech. August: 896-900. Trans., AIME, 228.

                     5)    Havlena, D. and Odeh, A.S., 1964. The Material Balance as an Equation of a
                           Straight Line. Part II - Field Cases. J.Pet.Tech. July: 815-822. Trans., AIME.,
                           231.
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