Page 140 - Design and Operation of Heat Exchangers and their Networks
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128   Design and operation of heat exchangers and their networks


          3.5.4.4 Wavy fins
          Dong et al. (2007) correlated their own experimental data from 11 wavy fin
          geometries and proposed the following correlations:

                             0:309    0:3703     0:25    0:1152
                  f ¼ 1:16Re    ð s f =h f Þ  ð 2a=s f Þ  ð l w =l s Þ  (3.302)
                j ¼ 0:0836Re  0:2309 ð s f =h f Þ 0:1284 ð 2a=s f Þ 0:153 ð l w =l s Þ 0:326  (3.303)
          where a is the wave amplitude, l w is the wavelength, and l s is the strip length
          of a wavy fin strip.
             Based on CFD calculation, Chennu (2016) presented the correlations for
          wavy fins as follows:
                                 0:322  2a   0:394   0:603

            f ¼ 9:827Re  0:705  h fs            l w      ð 100   Re   800Þ
                              s fs     s fs     2a
                                                                     (3.304)


                                0:264  2a   0:848   1:931
          f ¼ 10:628Re  0:359  h fs            l w     ð 1000   Re   15;000Þ
                             s fs    s fs      2a
                                                                     (3.305)
                                 0:312      0:192      0:432
                                      2a
             j ¼ 2:348Re  0:786  h fs           l w      ð 100   Re   800Þ
                              s fs    s fs      2a
                                                                     (3.306)

                               0:235  2a   0:288   0:553
           j ¼ 0:242Re  0:375  h fs           l w      ð 1000 < Re   15;000Þ
                            s fs    s fs      2a
                                                                     (3.307)
             More correlations based on their CFD simulation were summarized by
          Chennu (2018).


          3.6 Multistream parallel heat exchangers
          The multistream heat exchangers can be classified into two categories: One
          is the multichannel heat exchanger in which there is no thermal intercon-
          nection between the walls separating the fluids, such as shell-and-tube heat
          exchangers and plate heat exchangers. The other is multistream plate-fin
          heat exchanger. The mathematical model and its analytical solution for
          the thermal performance of parallel multistream plate-fin heat exchangers
          were first proposed by Kao (1961). Haseler (1983) defined a bypass efficiency
          that describes heat transfer between nonadjacent layers in a plate-fin heat
          exchanger to illustrate the bypass effect. For multichannel heat exchangers,
          a general solution of the temperature distributions was proposed by
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