Page 245 - Design and Operation of Heat Exchangers and their Networks
P. 245

Optimal design of heat exchanger networks  235


              in which
                                     T
                 0
               T ¼ t  0  t 0  ⋯ t 0
                 E    E,1 E,2   E,N
                                                                       T
                                          0
                                                    0
                  ¼ t 0 h,1  t 0 c,1  t 0 h,2  t 0 c,2  ⋯ t h,N E  t 0 c,N E  t M,1  t 0 M,2  ⋯ t 0 M,N M  (6.14)
                                       T
               T ¼ t  00  t  00  ⋯ t 00
                 00
                 E    E,1  E,2    E,N
                                                                       T
                  ¼ t 00  t 00  t 00  t 00  ⋯ t  00  t 00  t  00  t 00  ⋯ t 00  (6.15)
                      h,1  c,1  h,2  c,2  h,N E  c,N E  M,1  M,2  M,N M
                                       2                    3
                                        V 1               0
                                            ⋱
                                       6                    7
                                       6                    7
                                       6                    7
                                                V N E
                               V N N ¼  6                   7            (6.16)
                                                    1
                                       6                    7
                                       6                    7
                                                       ⋱
                                       4                    5
                                         0                1
                 To illustrate the interconnections among the heat exchangers, we use the
              following four matching matrices (The first three have been introduced in
              Section 3.6).
                 Interconnection matrix G: N N matrix whose elements g ij are defined as
                 the ratio of the thermal capacity rate flowing from channel j into channel
                 i to that flowing through channel i.
                                        0
                 Entrance matching matrix G : N N matrix whose elements g ik are
                                                0
                                                                         0
                 defined as the ratio of the thermal capacity rate flowing from the entrance
                 k to channel i to that flowing through channel i.
                                   00
                                       00
                 Exit matching matrix G : N  N matrix whose elements g li are defined as
                                                                 00
                 the ratio of the thermal capacity rate flowing from channel i to the exit l
                 to that flowing out of exit l.
                              000
                 Bypass matrix G : N  N matrix whose elements g 000 lk are defined as the
                                       0
                                  00
                 ratio of the thermal capacity rate flowing from entrance k to exit l to that
                 flowing out of exit l.
              We can write the energy balances at the inlets of N channels and at the net-
                            00
              work exits of N streams with these matrices as follows:
                                 N 0      N
                                X        X
                           t  0  ¼  g t +    g ij t 00  ð i ¼ 1, 2, …, NÞ  (6.17)
                                    0 0
                            E,i     ik k       E, j
                                k¼1       j¼1
                                N 0      N
                               X        X
                            00     000 0     00 00             00
                           t ¼    g t +     g t   ð l ¼ 1, 2, …, N Þ     (6.18)
                            l      lk k      li E,i
                               k¼1       i¼1
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