Page 120 - Air and gas Drilling Field Guide 3rd Edition
P. 120

5.5 Compressor Shaft Power Requirements       111




              For engineering calculations, Equation (5-1) is often simplified to the form
                                             P   R e T
                                               ¼                               (5-11)
                                                  S g
                                             g
                                                  R u
                                             R e ¼  ;                          (5-12)
                                                 m w
              where R e is the engineering gas constant for API standard condition air
              (53.36 lb-ft/lb- R, 29.31 N-m/N-K) and S g is the specific gravity of the particular

              gas used (for API standard condition air S g ¼ 1.0).

                 Equation (5-11) can be simplified further by defining R (lb-ft/lb- R, N-m/N-K)
              as the gas constant for any specified gas (e.g., air, natural gas, nitrogen). There-
              fore, the gas constant for any gas is approximately
                                                  R e
                                             R g ¼  :                          (5-13)
                                                  S g
                 Substituting Equation (5-13) into Equation (5-11) yields
                                             P
                                               ¼ R g T:                        (5-14)
                                             g
                 The specific volume and specific weight of a gas are related by
                                                  1
                                              v ¼ :                            (5-15)
                                                  g
                 Substituting Equation (5-15) into Equation (5-14) yields
                                             Pv ¼ R g T                        (5-16)

              or, specifically,
                                            Pv 1 ¼ R g T 1 :                   (5-17)
                 Using the definitions for a polytropic process given earlier and Equation (5-17),
              then Equation (5-10) can be reduced to
                                                       k   1
                                                 2            3
                                   ð 2
                                                    P 2  k    7
                                             R g T 1 6
                                     Pdv ¼       4            15:              (5-18)
                                    1        k   1  P 1
                 Again, using the definitions for a polytropic process and Equation (5-16), then
              a general relationship between P and T can be obtained. This is
                                              k   1

                                           P 2  k    T 2
                                                   ¼   :                       (5-19)
                                           P 1       T 1
                 Substituting Equation (5-19) into Equation (5-18) yields
                                 ð  2
                                         R g T 1 T 2   R g
                                   Pdn ¼          1 ¼      ðT 2   T 1 Þ:       (5-20)
                                  1      k   1 T 1    k   1
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