Page 109 - Design and Operation of Heat Exchangers and their Networks
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Steady-state characteristics of heat exchangers  97


                 For two-pass crossflow heat exchangers, Baclic (1990) summarized
              totally 32 possible flow arrangements with both fluids mixed in interpasses
              and their corresponding ε-NTU relationships. For more complicated multi-
              pass crossflow heat exchangers, in which each fluid is mixed either in the
              previous pass, or in the current pass, or between the previous and current
              passes, all the interpass temperatures are not the functions of the spatial coor-
              dinate x or y. So, we can treat the exchanger as a heat exchanger network in
              which each unit is a one-pass crossflow heat exchanger with uniform inlet
              temperatures of the two fluids flowing through the unit and calculate the
              interpass and outlet temperatures by the use of the general solution intro-
              duced in Section 6.1.

              3.3.4.2 Two-pass crossflow heat exchangers with at least one fluid
              unmixed throughout
              For two-pass crossflow heat exchangers, Baclic (1990) summarized totally
              40 flow arrangements with at least one fluid unmixed throughout. Their
              ε-NTU relationships have been summarized by Baclic (1990), which are
              expressed based on the following special functions:
                                             1
                                                    y
                                      KyðÞ ¼ ð 1 e Þ                    (3.154)
                                             y
                                              1
                                                 ð
                                      ν x, yÞ ¼ F 1 x, yÞ               (3.155)
                                       ð
                                              y
                                       ∗         xK yðÞ
                                      ν x, yð  Þ ¼ e                    (3.156)
                                              ∞
                                             X
                                                 n
                                    ð
                                   hx, y, zÞ ¼  z F n x, yÞ             (3.157)
                                                    ð
                                             n¼1
                                                 ð x
                                     1               2
                                                         0
                             μ x, yÞ ¼  F 1 y, xð  Þ   F y, x Þdx 0     (3.158)
                              ð
                                                     ð
                                                    0
                                      y           0
                                    ð x
                                  1
                                                 0
                                                             0
                                        ½
                                                     ð
                                            ð
                     μ x, y, z, ϕð  Þ ¼  F 0 z, ϕ x x ފF 0 y, x x Þdx 0  (3.159)
                      1
                                  x  0
                                         ð x
                                        1
                                                   0
                                                             0
                                             ð
                          μ x, y, z, ϕð  Þ ¼  F 0 z, ϕx ÞF 0 y, x x Þdx 0  (3.160)
                                                      ð
                           2
                                        x  0
              where the special function F n is defined by Romie (1987) as
                                     ∂F n x, yÞ
                                        ð
                                             ¼ G n  F n                 (3.161)
                                        ∂x
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