Page 268 - Standard Handbook Petroleum Natural Gas Engineering VOLUME2
P. 268

Material Balance and Volumetric Analysis   237


                 energies, Slider [ 1971 suggests beginning all material balance applications with
                 Equation 5-155.  With  the  use  of  Equation 5-155,  it is  not  necessary to  list
                 separate equations for the various drive mechanisms and conditions since this
                 one equation can be reduced to any of the individual cases. For reservoirs above
                 the  bubble point,  some of the  terms  in  Equation 5-155  become zero or else
                 cancel out: G = 0 since there is no free gas,  Gp, and N R, cancel out since the
                 gas production term is  equal to  the  total gas produce& Rd - q is  zero since
                 the gas in solution at any pressure is equal to the gas originally in solution.
                   For a reservoir with no initial free gas saturation or no initial gas cap, G = 0. If
                 there  is no water  encroachment, We = 0;  however,  the water production term
                 should remain, even if  there is no water drive, because connate water may  be
                 produced when  the reservoir pressure declines.
                   When  a  reservoir contains  free  gas,  the  pore  volume  expansion or  com-
                 pressibilities of the formation and water are insignificant compared to the free
                 gas terms. Since the gas compressibility is  about 100 times the compressibility
                 of  the water and formation, a gas  saturation of only 1% may  provide as much
                 energy as the water  and formation compressibility terms. Thus, when  the gas
                 saturation is substantial the change in pore volume is  insignificant.
                            Material Balance for  Soiution-Gas Drive Reservoirs

                   A  schematic representation  of  material balance equations for  solution-gas
                 reservoirs, when the change in pore volume is negligible, is shown in Figure 5144.
                 When  these  reservoirs are producing  above the  bubble  point  or  saturation
                 pressure, no gas  is liberated and production occurs by  expansion of  liquids in
                 the  reservoir.  When  reservoir  pressure drops below  the  bubble  point, gas is
                 liberated in the reservoir and will be produced with the  oil.
                 Liquld Expansion

                   For some very large reservoirs (often with limited permeability), production
                 may  occur  for  extended periods  by  expansion  of  liquids in  the  reservoir. If














                                                                       Free  Gas

                 for  P<Ps

                                       Pi                         P < Ps

                 Flgure 5-1 44.  Schematic  of  material balance equations for  a solution-gas-
                 drive reservoir [ 1971.
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