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                       352                       Applied Process Design for Chemical and Petrochemical Plants

                                                                                               1
                                                                             tropic to actual bhp. For a large reciprocating compressor
                                                                             system, e o   60—70% and 50—65% for small machines. Refer
                                                                             to the section on compressors for detailed data. e o is not just
                                                                             the mechanical efficiency of the compressor; it is the prod-
                                                                             uct of indicated and mechanical compressor efficiencies. 1

                                                                               Actual Enthalpy. The actual enthalpy of compressed refrig-
                                                                             erant to account for deviation from isentropic compression
                                                                             is referenced to Figure 11-48A, point 2.
                                                                               Correct enthalpy corresponding to isentropic point 2 is:  1

                                                                                                           Q
                                                                                               h 2      h 1
                                                                             h 2  1corr.2     h 1      a  b                (11-9)
                                                                                                  e o      W
                                                                               For large tonnage requirements the heat loss, Q, is often
                                                                             negligible as far as determining h 2 (corr.) is concerned, but
                                                                             it must be included as far as total tonnage requirements are
                                                                             concerned.

                                                                               Refrigerant Flow Rate. Refer to Figure 11-48A.

                                                                                            200
                                                                             lb>min>TR                                    (11-10)
                                                                                          h 1      h 3
                                                                               For subcooled refrigerant, Figure 11-48B,

                                                                                            200
                                                                             lb>min>TR                                    (11-11)
                                                                                          h 1      h 3
                       Figure 11-48. Isentropic compression refrigeration cycles.
                                                                               Note that the temperature at this h 3 is lower than when no
                                                                             subcooling exists.

                                                                                             200
                                                                             cfm per TR     a     b1v 1 2  , at compressor intake  (11-12)
                                                                                           h 1      h 3
                                  1
                         Horsepower. From Figure 11-48A or 11-48B.
                                                                               Heat Removed by Condenser.
                                          200   h 2   h 1
                       Theoretical HP>TR       a      b              (11-6)          h 2      h 3
                                         42.42  h 1   h 3                        200a       b, Btu>ton min                (11-13)
                                                                                     h 1      h 3
                                                                               For Economizer System. See Figure 11-48C. Refrigerant flow
                                                        1k 12>k
                                                     P 2
                                         0.873 k P 1  v 1 ca  b    1d        in the second (or later) stage is the sum of first-stage weight
                                                     P 1
                       Theoretical HP>TR                         ,   (11-7)  flow plus the weight flow of the vapor flashed from the econ-
                                              1k   12 1h 1   h 3 2                 19
                                                                             omizer.
                                                                               Lb flashed gas from economizer/lb vapor from evapora-
                       for isentropic compression. For polytropic compression, k is
                                                                             tor
                       replaced by n,
                       where,                                                      h 3     h 5
                                                                                 h 1c      h 3
                           n                  k
                        a     b   1efficiency2 a  b                  (11-8)
                         n   1              k   1                              When economizer vapors are mixed with the compressor
                                                                             vapors, the temperature from this mixing point on is lower
                         Brake Horsepower. Bhp   theoretical hp/e o , where e o is the  to the next stage of compression than if the economizer had
                       overall compression efficiency, the ratio of theoretical isen-  not been used. 19
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