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Guo, Boyun / Computer Assited Petroleum Production Engg 0750682701_chap15 Final Proof page 229 22.12.2006 6:14pm




                                                                            WELL PROBLEM IDENTIFICATION  15/229
                       . Near wellbore damage/stimulation          r w  ¼ wellbore radius
                       . Rate-dependent skin                       S  ¼ total skin factor.
                       . Boundary identification
                       . Partial penetration effect on flow         Horizontal Linear Flow. For hydraulically fractured
                       . Effective fracture length               wells, the horizontal linear flow can be mathematically
                       . Effective fracture conductivity         described in consistent units as
                       . Dual-porosity characteristics (storativity and transmis-  " s ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi  #
                         sivity ratios)                                  qBm    pk y t
                                                                 p wf ¼ p i          þ S ,           (15:2)
                       The theoretical basis of pressure transient data analysis is  2pk y h  fmc t x 2 f
                       beyond the scope of this book. It can be found elsewhere
                       (Chaudhry, 2004; Horne, 1995; Lee et al., 2003). Modern  where x f is fracture half-length and k y is the permeability
                       computer software packages are available for data anal-  in the direction perpendicular to the fracture face.
                       yses. These packages include PanSystem (EPS, 2004) and  Vertical Radial Flow. For horizontal wells as depicted
                       F.A.S.T. WellTest (Fekete, 2003). The following subsec-  in Fig. 15.2, the early-time vertical radial flow can be
                       tions briefly present some principles of data analyses that  mathematically described in consistent units as
                       lead to deriving reservoir properties directly affecting well
                       productivity.                             p wf ¼ p i    qBm  ln  k yz t  þ 2S þ 0:80907 ,  (15:3)
                          Reservoir Pressure. Reservoir pressure is a key param-  4pk yz L  fmc t r 2 w
                       eter controlling well deliverability. A simple way to deter-  where L is the horizontal wellbore length and k yz is the
                       mine the magnitude of initial reservoir pressure may be  geometric mean of horizontal and vertical permeabilities,
                       the Horner plot of data from pressure buildup test if  that is,
                       the reservoir boundary was not reached during the test.  p ffiffiffiffiffiffiffiffiffi
                       If the boundary effects are seen, the average reservoir  k yz ¼  k y k z :    (15:4)
                       pressure can be estimated on the basis of the extrapolated  Horizontal Pseudo-Linear Flow. The pseudo-linear
                       initial reservoir pressure from Horner plot and the MBH  flow toward a horizontal wellbore can be mathematically
                       plot (Dake, 2002).                        described in consistent units as
                          Effective Permeability. The effective reservoir perme-
                       ability that controls the well’s deliverability should be  " s ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi  #
                       derived from the flow regime that prevails in the reservoir  p wf ¼ p i    qBm  4pk y t  þ S :  (15:5)
                                                                            ð
                       for long-term production. To better understand the flow  2pk y h   Z w Þ  fmc t L 2
                       regimes, the commonly used equationsdescribingflow in oil
                       reservoirs are summarized first in this subsection. Similar  Horizontal Pseudo-Radial Flow. The pseudo-radial
                       equations for gas reservoirs can be found in Lee et al. (2003).  flow toward a horizontal wellbore can be mathematically
                          Horizontal Radial Flow. For vertical wells fully pene-  described in consistent units as
                       trating nonfractured reservoirs, the horizontal radial flow  qBm        k h t
                       can be mathematically described in consistent units as  p wf ¼ p i    ln  2  þ 2S þ 0:80907 :  (15:6)
                                                                         4pk h h  fmc t r w
                               qBm      k h t
                       p wf ¼ p i    ln      þ 2S þ 0:80907 ,  (15:1)  For vertical wells fully penetrating nonfractured reser-
                               4pk h h  fmc t r 2 w              voirs, it is usually the average (geometric mean) of hori-
                       where                                     zontal permeabilities, k h , that dominates long-term
                         p wf ¼ flowing bottom-hole pressure     production performance. This average horizontal perme-
                          p i ¼ initial reservoir pressure       ability can be derived from the horizontal radial flow
                          q ¼ volumetric liquid production rate  regime. For wells draining relatively small portions of
                          B ¼ formation volume factor            hydraulically fractured reservoir segments, it is usually
                          m ¼ fluid viscosity                    the permeability in the direction perpendicular to the frac-
                          k h ¼ the average horizontal permeability  ture face that controls long-term production performance.
                          h ¼ pay zone thickness                 This permeability can be derived from the horizontal lin-
                           t ¼ flow time                         ear flow regime. For horizontal wells draining relatively
                          f ¼ initial reservoir pressure         large portions of nonfractured reservoir segments, it is usu-
                                                                 ally again the geometric mean of horizontal permeabilities
                         c t  ¼ total reservoir compressibility

                                         z
                                                                  L
                                                                                       h
                                              x
                                       y                       Z w




                                         z
                                                                                       h
                                              y
                                                               Z
                                       x                        w

                                               Figure 15.2 Notations for a horizontal wellbore.
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