Page 130 - Air and Gas Drilling Manual
P. 130

4-16    Air and Gas Drilling Manual
                               compression, and delivery of the gas under conditions which are assumed to  be ideal
                               (absence of fluid or mechanical friction, and mechanically reversible).












                               Figure 4-13: Basic pressure-volume diagram.

                                   The total shaft work, W s  (ft-lb/lb),  required for compression can be written as
                                            V 2 2  V 1 2        2         
                                      W =       −        Pv   − ∫  P dv −  P v          (4-6)
                                                        
                                        s             +  2  2          1  1 
                                            2 g    2 g          1
                               or

                                            V  2  V  2          1         
                                      W =    2  −  1  +  2   + ∫  P dv −  P v          (4-7)
                                                         Pv
                                        s
                                            2 g    2 g     2   2       1  1 
                               where W s is the total shaft work (ft-lb/lb),
                                    V 1  is the velocity of the gas entering the compressor (ft/sec),
                                    V 2  is the velocity of the gas exiting the compressor (ft/sec),
                                                                   2
                                    g is the acceleration of gravity (32.2 ft/sec ).
                                   Equation 4-6 can be rewritten as
                                            V 1 2  V 2 2                2
                                      W +      −     +  Pv −  P v  = −  ∫  P dv          (4-8)
                                        s
                                            2 g   2 g   1  1   2  2     1
                                                                        n
                                                                  n
                                                                             n
                                   Assuming a polytropic process, where  Pν  =  P ν  =  Pν  =  constant, and the
                                                                11    22
                               simplest polytropic process where the exponent term n  ≈  k, where k  is  the ratio of
                               specific heats for the gas involved in the process (e.g., for air, k = 1.4), Equation 4-8
                               can be written as
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