Page 177 - Air and gas Drilling Field Guide 3rd Edition
P. 177

168     CHAPTER 7 Reverse Circulation Models




                          and average annual temperatures for sea level and various elevations above sea
                          level can be approximated for most of North America by midlatitudes data given
                          in Tables 5-1a and 5-1b. These reference pressures are denoted as p r and t r . For
                          engineering calculations, the actual atmospheric pressure and temperature of the
                          air entering a primary compressor(s) are p at and t at and can be approximated as
                                                                                            (7-2)
                                                          p at   p r
                                                          t at   t r ;                      (7-3)
                                                                    2
                          where p at is atmospheric pressure (psia, N/cm abs), p r is the reference atmo-
                                                    2
                          spheric pressure (psia, N/cm abs), t at is atmospheric pressure (psia, N/cm 2


                          abs), and t r is the reference atmospheric temperature ( F, C). Also see Appendix
                          B for more detailed plots for atmospheric conditions for North America midlati-
                          tudes. Similar data as that given in Tables 5-1a and 5-1b and Appendix B for North
                          America midlatitudes can be obtained for most other continents and latitudes
                          around the world.
                             The aforementioned pressures and temperatures in field units must be con-
                          verted to units consistent with Equations (5-11) and (7-1). These are

                                                          P g ¼ P r                         (7-4)
                                                          T g ¼ T r ;                       (7-5)
                                                                         2
                                                                                  2
                          where P r is the reference atmospheric pressure (lb/ft abs, N/m abs) and T r is

                          the absolute atmospheric reference temperature ( R, K).
                             Substituting Equations (7-2) and (7-3) into Equation (5-11), the specific weight
                          of the gas (air) g g entering the compressor(s) is
                                                          P g S g  P r S g
                                                      g ¼     ¼     ;                       (7-6)
                                                      g
                                                         R e T g  R e T r
                                                        3
                                                              3
                          where g g is specific weight (lb/ft , N/m ), R e is the engineering gas constant

                          (53.36 ft-lb/lb- R, 29.31 N-m/N-K), and S g is the specific gravity of the gas (S g ¼
                          1.0 for air at standard conditions). The weight rate of flow of the gas, _ w g through
                          the compressor is
                                                         _ w g ¼ g Q g ;                    (7-7)
                                                              g
                          where _ w g is the weight rate of flow of gas (lb/sec, N/sec) and Q g is the volumet-
                                                                          3            3
                          ric flow rate of air into the circulation system (actual ft /sec, actual m /sec).
                             If the gas for the drilling operation is natural gas from a pipeline and the pres-
                          sure and temperature of the gas in the pipeline are p pl and t pl , then the pressure
                          and temperature of the gas entering either directly into the circulation system or
                          to the booster compressor are

                                                          P g ¼ P pl                        (7-8)
                                                          T g ¼ T pl ;                      (7-9)
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