Page 303 - Air and Gas Drilling Manual
P. 303

7-12    Air and Gas Drilling Manual
                                    γ mixbh is the mixture specific weight at the bottom of the annulus (lb/ft ).
                               Equation 7-33 must  be solved by trial and error techniques since γ mixai depends  on
                               the pressure P bh.  Note  that  this  equation  does  not  account  for  friction  flow  loss
                               through the orifices and nozzles.                       3
                                   For fluid mixtures that are nearly all gas (with little  incompressible  fluid  and
                               rock cuttings) and subsonic flow conditions,  the pressure above the drill  bit  inside
                               the drill string is determined from [1]
                                                           2        k+ 1      2
                                           k            P   k    P   k     ˙  g
                                                                            w 
                                                         ai
                                                                  ai
                                      2g        P γ bh      −        =       (7-34)
                                                 bh
                                           k −  1       P     P        A bi 
                                                                  bh
                                                         bh
                               where k is the ratio of specific heats for the gas (e.g., for air k = 1.4 and for natural
                                    gas k = 1.28).
                                                                                       3
                                    γ bh is the specific weight of the gas at the bottom of the annulus (lb/ft ).
                               Equation 7-34 must  be solved by trial and error for P bh.   Note that  Equation  7-34
                               does not account for friction flow loss through the single drill bit orifice.
                                  The above equations will generally yield results that show that for most  practical
                               parameters the annulus bottomhole pressure, P bh, differs very little  from the pressure
                               above the drill bit inside the drill  string,  P ai.   Therefore, it  can usually be assumed
                               that
                                      P bh  ≈  P ai                                    (7-35)
                                 7.2.4 Two-Phase Flow in the Annulus
                                   The downward flow condition  in  the  annulus  is  two  phase.    The  differential
                               pressure, dP, occurs over the incremental distance of dh.  This  differential pressure
                               can be approximated as
                                                         2    
                                      dP = γ mix    1  −  fv  p)    dh             (7-36)
                                                        h (
                                                   2 gD −  D  

                               where D h  is the inside diameter of the annulus (ft) (the borehole),
                                    D p is the outside diameter of the drill string (pipe and collars) (ft).
                                   The two phase flow of gas and incompressible fluid down the annulus space to
                               the bottom of the well can be described by a mixed specific weight term which is  a
                               function of position in the annulus.  This mixed specific weight term is

                                                  w ˙  g  +  w ˙  m
                                      γ   =                                            (7-37)
                                       mix
                                               P g    T av  
                                                     Q +  Q m
                                                         g
                                               P    T g 
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