Page 110 - Introduction to Petroleum Engineering
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WELL PRODUCTIVITY                                                95

                     1.00

                                                 Saturation
                     0.80
                                                  “shock”
                    Water saturation  0.60


                     0.40

                     0.20


                     0.00
                        0.00     0.20     0.40     0.60     0.80     1.00
                                         Normalized position

              FIgURE 5.11  Water saturation profile when the front is halfway through the sample.

            called a saturation shock or a shock front. Ahead of the shock front, water saturation
            is constant and equal to initial water saturation S . Behind the front, water saturation
                                                  wi
            gradually increases to S =−  S  at the inlet position. Water breakthrough corre-
                                  1
                               w
                                      or
            sponds to arrival of the front at the outlet position. After breakthrough, the saturation
            profile continues to rise, asymptotically approaching S =−  S .
                                                          1
                                                              or
                                                       w
              Welge’s method was primarily intended to provide a graphical means for
              estimating oil production for water or gas flooding. Such an approach was satisfac-
            tory at the time. Today, software is available that uses numerical techniques to apply
            the Buckley–Leverett–Welge method.
            5.6  WELL PRODUCTIVITY

            Production of fluid from a well can be quantified using the concept of well produc-
            tivity. Consider the case of radial flow into a vertical well. Volumetric flow rate q  for
                                                                            ℓ
            phase ℓ is proportional to pressure differential Δp so that

                                        q =  PI ×∆ p                      (5.16)
                                         
            where the proportionality factor is the productivity index PI. The pressure differential
            is the difference between reservoir pressure and flowing wellbore pressure, or

                                       ∆p =  p −  p fwb                   (5.17)
                                             res
            The productivity index terms are illustrated in Figure 5.12. Fluid flows from the res-
            ervoir, through perforations in the casing into the wellbore, and up the tubing to the
            surface. The pressure differential is greater than zero (∆p > 0) for production wells
            and less than zero (∆p < 0) for injection wells. In the case of fluid injection, the term
            injectivity index is used.
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