Page 189 - Air and gas Drilling Field Guide 3rd Edition
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180     CHAPTER 7 Reverse Circulation Models




                                                      2              3 2
                                                              1
                                                      6              7
                                                   f ¼  6            7  :                  (7-52)
                                                            D i
                                                      4              5
                                                       2 log    þ 1:14
                                                             e
                          For follow-on calculations for flow in the drill string, the absolute roughness for
                          commercial steel drill pipe, e p ¼ 0.0005 ft or e p ¼ 0.0002 m, will be used for
                          the inside surfaces of the drill pipe and drill collars.
                             Equations (7-46), (7-47), (7-51), and (7-52) can be used in sequential
                          calculation steps starting at the top of the inside of the drill string and
                          continuing for each subsequent change in cross-sectional area in the inside of
                          the drill string until the pressure above the drill bit inside of the drill string is
                          determined.
                             There is a single water course in reverse circulation drill bits. Using Equation
                          (7-53), the pressure at the bottom of the inside of the drill string P ai is obtained.
                          The pressure at the bottom of the annulus P bh can be obtained by trial and error
                          using the expression
                                                                    k þ 1
                                                      2                 3
                                                            2
                                                                                  2
                                             k           P ai  k  P ai        _ w g
                                        2g       P bh g 4             k 7         :        (7-53)
                                                      6
                                                                        5 ¼
                                                    bh
                                           k   1        P bh    P bh         A bi
                             These equations will generally yield results that show that the annulus bottom
                          hole pressure P bh differs very little from the pressure above the drill bit inside the
                          drill string P ai for most practical parameters. Therefore, it can usually be assumed
                          that
                                                         P bh   P ai :                     (7-54)
                             The flow in the annulus is single-phase flow (air or gas). Setting Q m ¼ 0in
                          Equation (7-37) yields
                                                        2            3
                                                        6      _ w g  7
                                                        6            7
                                                    dP ¼
                                                        4            5
                                                           P g  T av
                                                                   Q g
                                                           P    T g
                                            8                             9
                                                                        32
                                                           2
                                                              P g  T av
                                            >                             >
                                            >                             >
                                                                      Q g
                                            >                             >
                                                      f    6  P   T g   7
                                            <                             =
                                              1             6           7  dh:             (7-55)
                                                           4  p  2   2  5
                                            >    2gD h   D p    D   D     >
                                            >                             >
                                                             4
                                            >                    h   p    >
                                            :                             ;
                          Separating variables in Equation (7-59) yields
                                                       P bh
                                                          dP
                                                      ð         ð H
                                                              ¼   dh;                      (7-56)
                                                         B a PðÞ
                                                       P in      0
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