Page 264 - Design and Operation of Heat Exchangers and their Networks
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Optimal design of heat exchanger networks  253


                 The position where the heat input is zero is the pinch.
                 The problem table provides a simple framework for numerical analysis.
              For simple problems, it can be quickly evaluated by hand. For larger prob-
              lems, it is easily implemented on the computer. With the problem table
              algorithm, the engineer has a powerful targeting technique at their finger-
              tips. Data can be quickly extracted from flow sheets and analyzed to see
              whether the process is nearing optimal or whether significant scope for
              energy saving exists.


              6.3.2 Composite curves
              The composite curves were first used by Huang and Elshout (1976).
              A similar concept is the composite line in the available energy diagram
              applied by Umeda et al. (1978). To structure the composite curves, we draw
              the hot and cold process streams on a temperature-heat content (enthalpy)
              diagram. Starting from the individual streams, one composite curve is con-
              structed for all hot streams in the process and another for all cold streams by
              simple addition of heat contents over the temperature ranges in the problem.
              The overlap between the two composite curves represents the maximum
              amount of heat recovery possible within the process. The “overshoot” of
              the hot composite curve represents the minimum amount of required exter-
              nal cooling duty, and the “overshoot” of the cold composite curve repre-
              sents the minimum amount of required external heating duty.
                 To draw the composite curves, let j 1 and j 2 indicate the maximum and
              minimum temperature levels of the hot streams; k 1 and k 2 indicate those of
              the cold streams, respectively, so that
                         n               o          n               o
                   ¼ max t 0  , t 0  , …, t 0  ¼ min t  00  , t  00  , …, t  00  (6.71)
                           h,1  h,2   h,N h           h,1  h,2   h,N h
                 t j 1                     , t j 2
                        n                o          n                 o
                  ¼ max t 00  , t  00  , …, t 00  ¼ min t 0  , t 0  , …, t 0  (6.72)
                          c ∗,1  c ∗,2  c ∗,N c       c ∗,1  c ∗,2  c ∗,N c
               t k 1                       , t k 2
                 Then, we can calculate the enthalpy flow rates of the hot and cold
              streams at the temperature levels t j with Eq. (6.73):
                               j 2  1          k 2  1
                               X               X
                         H h, j ¼  ΔH h,i , H c,k ¼  ΔH c,i + Q CU,min   (6.73)
                                i¼j             i¼k

              to get the coordinates of the composite curve of the hot streams (t j , H h,j )
              (j¼j 1 , j 1 +1, …, j 2 ) and those of the cold streams (t k – Δt m , H c,k )(k¼k 1 ,
              k 1 +1, …, k 2 ), respectively, and draw the polyline composite curves.
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