Page 387 - Design and Operation of Heat Exchangers and their Networks
P. 387

370   Design and operation of heat exchangers and their networks


                           j = 1         2         3         i = m = 4
           i = 1   x in,1                  k = 1                       x out,1

           i = 2   x out,2  k = 2  x in,2 x out,3  k = 3               x in,3

           i = 3   x in,4              k = 4        x out,4  x in,5  k = 5  x out,5

           i = n = 4  x out,6    k = 6      x in,6 x out,7  k = N f  = 7  x in,7
          Fig. 7.12 Arrangement of the streams, layers, and sections in a plate-fin heat exchanger.


             Consider a multistream parallel channel plate-fin heat exchanger that has
                                  00
             0
          N stream entrances and N stream exits and is well thermally insulated. We
          divide the exchanger into m sections along the exchanger length according
          to the inlet and outlet positions of the streams (see Fig. 7.12 as an example).
          Section j consists of n j layers and n p,j plates. A layer in a section is named as a
          channel. Thus, the total number of channels is
                                           m
                                          X
                                      M ¼     n j                    (7.215)
                                           j¼1
             The number of the plates depends on the layer arrangement. It is con-
          venient to set the maximal length of the arrays for the plates with n p,j ¼n j +1.
          Thus, the total number of the plates is
                                       m
                                      X
                                 M p ¼   n p, j ¼ M + m              (7.216)
                                      j¼1
             The exchanger operates at first at a steady-state operation condition
          denoted with “^” and then undergoes a transient process caused by distur-
          bances in supply temperatures and flow rates around the steady-state oper-
          ation condition. The mathematical description can be obtained from energy
          balances of the fluids, separating plates and fins. The resulting governing
          equations for section q
                               j 1
                               X
                  q ¼ i, jðÞ ¼ i +  n k , i ¼ 1,2,…, n j ;j ¼ 1,2,…,m  (7.217)
                               k¼1
          can be written as follows:
                                                         0           1
                                                           1
                                                           ð
                 ∂t ij  _  ∂t ij  U p, ij
              C ij  + C ij  ¼      t p, ij + t p,i +1, j  2t ij + U f, ij  @  t f, ij dy t ij  A
                 ∂τ      ∂x    2
                                                           0
                                                                     (7.218)
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