Page 126 - Design and Operation of Heat Exchangers and their Networks
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114   Design and operation of heat exchangers and their networks


          solution of the correction factor for the logarithmic mean temperature
          difference:
                                                 2
                                       ln 1 + CN Þ
                                         ð
                                   F          2                      (3.216)
                                          CN
          where the criterion number CN is defined by
                                              r ffiffiffiffiffiffiffiffi
                                                πA c
                                  CN ¼ 2NTU                          (3.217)
                                                 A
                                             kA
                                                                     (3.218)
                                   NTU ¼ p   ffiffiffiffiffiffiffiffiffiffiffiffi
                                             _ _
                                             C h C c
          in which A is the total heat transfer surface area and the cross-sectional area
                                        _
                                    _
          A c ¼hs. For n>10 and 0.2 C h =C c  5, Eq. (3.216) agrees very well with
          the exact solution developed by Bes and Roetzel (1992b) with an analytical
          method for the accurate calculation of the temperature changes in counter-
          flow spiral heat exchangers, in which the spiral is composed of circular arc
          profiles with the centers of curvature on the angles of an equilateral triangle.
             An alternative channel arrangement of a spiral heat exchanger is shown in
          Fig. 3.10. By neglecting the heat transfer in the open area at the center and
          expressing the radius with

                                                 θ
                                 r ¼ r 0 + s h + s c Þ               (3.219)
                                        ð
                                                2π
          we can apply the previous energy equations in the three regions as
             The innermost region 1, 0<θ<π:

                 _  dt c θðÞ
                                    ð
                             ð
                 C c     + kh r + s c Þφ r + s c Þ t h θ +2πð½  Þ t c θðފ ¼ 0  (3.220)
                     dθ



                                                          .
                                            r         t  , C
                                       t h,in  q       c,in  c
                           .        s       r
                          C h , t h,out      0
                                                       t c,out



          Fig. 3.10 An alternative channel arrangement in a spiral heat exchanger, turns n¼3.
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