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204                                                  Reservoir Drive Mechanisms


          stored in the system. Three sets of the fluid initial conditions can be distinguished
          for an oil, and reservoir and production behaviour may be characterised in each
          case

           Drive Mechanism                     Fluid Initial Condition

           Solution gas drive (or depletion drive)  Undersaturated oil (no gas cap)
           Gas cap drive                       Saturated oil with a gas cap
           Water drive via injection or with a large  Saturated or undersaturated oil
             underlying aquifer


          9.2.1. Solution gas drive (or depletion drive)
          Solution gas drive occurs in a reservoir which contains no initial gas cap or
          underlying active aquifer to support the pressure and therefore oil is produced by
          the driving force due to the expansion of oil and connate water, plus any
          compaction drive. The contribution to drive energy from compaction and connate
          water is small, so the oil compressibility initially dominates the drive energy.
          Because the oil compressibility itself is low, pressure drops rapidly as production
          takes place, until the pressure reaches the bubble point.
             The material balance equation relating produced volume of oil (N p stb) to the
          pressure drop in the reservoir (DP)isgivenby

                                      N p B o ¼ NB oi C e DP
          where B o is the oil formation volume factor at the reduced reservoir pressure (rb/stb);
          B oi the oil formation volume factor at the original reservoir pressure (rb/stb); C e
                                                                          1
          the volume averaged compressibility of oil, connate water and rock (psi ); N the
          STOIIP (stb).
             Once the bubble point is reached, solution gas starts to become liberated from
          the oil, and since the liberated gas has a high compressibility, the rate of decline of
          pressure per unit of production slows down.
             Once the liberated gas has overcome a critical gas saturation in the pores, below
          which it is immobile in the reservoir, it can either migrate to the crest of the
          reservoir under the influence of buoyancy forces, or move toward the producing
          wells under the influence of the hydrodynamic forces caused by the low pressure
          created at the producing well. In order to make use of the high compressibility of
          the gas, it is preferable that the gas forms a secondary gas cap and contributes to the
          drive energy. This can be encouraged by reducing the pressure sink at the producing
          wells (which means less production per well) and by locating the producing wells
          away from the crest of the field. In a steeply dipping field, wells would be located
          down-dip. However, in a field with low dip, the wells must be perforated as low as
          possible to keep away from a secondary gas cap (Figure 9.2). The problem of water
          coning, discussed in Section 10.2, Chapter 10 is a constraint on just how low down
          the perforation can be placed without producing excessive amounts of water.
             The characteristic production profile for a reservoir developed by solution gas
          drive is shown in Figure 9.3.
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