Page 241 - Standard Handbook Petroleum Natural Gas Engineering VOLUME2
P. 241

410    Reservoir Engineering


                                             Productivlty Index
                      The productivity index, J, is  a measure of  the  ability of  a well  to  produce
                    hydrocarbon liquids:


                             9.
                       J, =-                                                      (5-128)
                           P.  - Pllf
                    where    is  the flow rate  of  oil  in  stock-tank barrels of  oil per  day,  p,  is  the
                    external pressure in psi, Pw, is  the flowing bottomhole pressure in psi, and the
                    quantity (p, - p,)   is  referred to as the  pressure drawdown. Because the flow
                    rate in this case is in STB/D,  the oil productivity index u,)  has units of  STB/
                    D/psi.  Since only q and pwr can be measured directly, p,  is  commonly replaced
                    with   which  can be  determined from pressure transient testing.
                      After the well has been shut in for a period of  time (usually at least 24 to 72
                    hours  or longer  depending  on  reservoir characteristics), the  well  is  put  on
                    production at a low rate with a small choke. The rate of production is recorded
                    as a function of  flow time. When the production rate has stabilized, the flow
                    rate is increased by  increasing the choke, and flaw rate is monitored with time.
                    This process is repeated until a series of measurements has been recorded [19].
                      In order to attain a stabilized productivity index, a minimum time is required
                    after each individual flow-rate change. This time can be  approximated by  two
                    equations [66,197]:


                                                                                  (5-129)



                                                                                  (5-1  30)

                    where t,  is  the stabilization time in hours, k is the permeability in md, I$ is the
                    porosity as a fraction, p is viscosity in cp, c, is  total compressibility in psi-’,  A
                    is  area in ft*, and re. is  the  external radius in feet which  should be based on
                    the distance to  the farthest drainage boundary for the well.  For  large systems
                    or reservoirs with low permeability, very long stabilization times may be required.
                       Equation 5-128 assumes that  productivity index does not  change with  flow
                     rate or time, and in some wells  the flow rate will  remain proportional to the
                     pressure drawdown over  a wide  range  of  flow rates.  However,  in  many  wells,
                     the direct relationship is  not linear at high  flow rates as shown in Figure 5-129.
                     The causes for the deviation in the straight-line behavior can include insufficient
                     producing times at each rate, an increase in gas saturation near the wellbore
                     caused by  the pressure drop in  that  region, a decrease in permeability of  oil
                     due  to  the  presence of  gas,  a  reduction  in  permeability due  to  changes in
                     formation compressibility, an increase in oil viscosity with pressure drop below
                     the bubble point, and possible turbulence at high rates of  flow.
                       A plot of  oil production rate versus bottomhole pressure, termed the inflow
                     performance relationship (IPR), was proposed as a method of analysis of flowing
                     and  gas-lift wells  [223].  Vogel  [224]  calculated dimensionless IPR  curves for
                     solution  gas  reservoirs  that  covered  a  wide  range  of  oil  PVT  and  relative
                     permeability characteristics. From computer simulations, Vogel [224] showed that
   236   237   238   239   240   241   242   243   244   245   246