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P r o c e s s I n t e g r a t i o n f o r I m p r ov i n g E n e r g y E f f i c i e n c y   59


                     Next, the sums of the segment CPs (heat capacity flow rates) in each
                     interval are calculated; then that sum is multiplied by the interval
                     temperature difference (i.e., the difference between the TBs that
                     define each interval). This calculation is also illustrated in Table 4.3.

                     Step 4
                     The Problem Heat Cascade shown in Figure 4.14 has a box allocated
                     to each temperature interval; each box contains the corresponding
                     interval enthalpy balances. The boxes are connected with heat flow
                     arrows in order of descending temperature. The top heat flow
                     represents the total hot utility provided to the cascade, and the
                     bottom heat flow represents the total cold utility. The hot utility flow
                     is initially assumed to be zero and this value is combined (summed)
                     with the enthalpy balance of the top cascade interval to produce the
                     value for the next lower cascade heat flow. This operation is repeated
                     for the lower temperature intervals and connecting heat flows until
                     the bottom heat flow is calculated, resulting in the cascade shown in
                     Figure 4.14(a).
                     Step 5
                     The resulting heat flow values in the cascade are examined, and a
                     feasible heat cascade is obtained; see Figure 4.14(b). From the
                     cascading heat flows, the smallest value is identified; if it is
                     nonnegative (i.e., positive or zero), then the heat cascade is
                     thermodynamically feasible. If a negative value is obtained then a
                     positive utility flow of the same absolute value has to be provided at



                     (a)            HOT UTILITY (b)           HOT UTILITY
                     245 °C            0 kW    245 °C           750 kW
                          ΔH = 150 kW               ΔH = 150 kW
                     235 °C        150 kW      235 °C       900 kW
                          ΔH = −600 kW             ΔH = −600 kW
                     195 °C       −450 kW      195 °C       300 kW
                          ΔH = 100 kW               ΔH = 100 kW
                     185 °C       −350 kW      185 °C       400 kW
                          ΔH = −400 kW             ΔH = −400 kW    T HOT PINCH  = 150°C
                                                         *
                     145 °C       −750 kW      145 °C   T PINCH  0 kW
                                                                   T COLD PINCH  = 140°C
                          ΔH = 1400 kW             ΔH = 1400 kW
                      75 °C       −650 kW       75 °C      1400 kW
                          ΔH = −200 kW             ΔH = −200 kW
                      35 °C       −450 kW       35 °C      1200 kW
                          ΔH = −200 kW             ΔH = −200 kW
                      25 °C           250 kW    25 °C          1000 kW
                                    HOT UTILITY              HOT UTILITY
                          (a) Initial cascade      (b) Feasible cascade
                     FIGURE 4.14  Heat Cascade for the process data in Table 4.2.
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