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122    Chapter 5 Heat exchanger network analysis




             Without any heat exchange between the hot and the cold streams, the annual cost of utility requirement
             (C op,annual ) is computed from the unit cost of the hot and cold utility i.e. C h , and C c , respectively
             multiplied by the hours of operation per annum (t ann )
                                                                                           (5.3)
                                      C op;annual ¼ðq h   C h þ q c   C c Þ  t ann
                When the hot stream is used to preheat the cold stream, the corresponding energy savings in the
             recovery heat exchanger (q rec ) is obtained at the expense of an investment (C ex ) which is a function of
             the heat exchanger area (A ex ) computed for a counterflow exchanger as
                                                       q rec
                                                                                           (5.4)
                                           A ex ¼
                                                U ex DT LMTDcounterflow
                The above expression considers the LMTD correction factor (multiplier to DT LMTDcounterflow )tobe
             close to unity. However the same may be incorporated, if multipass exchangers are used.
                Following the nomenclature depicted in Fig. 5.2,

                                                TS h   T c;rec   T h;rec   TS c

                                                        TS h   T c;rec                     (5.5)
                               DT LMTDcounterflow ¼
                                                     ln
                                                        T h;rec   TS c
             where T c,rec and T h,rec refer to the respective exit temperatures of the cold and the hot streams from the
             recovery exchanger.
                Overall heat transfer coefficient (U ex ) can be obtained from the convective heat transfer coefficient
             for the cold (h c ) and the hot fluid (h h ) as discussed in Chapters 2e4.
                The heat recovery (q rec )in Eq. 5.4 is limited by the approach temperature ðDT min Þ, the temperature
             difference between the hot and the cold stream in the exchanger. For constant heat load (q h and q c )of
             the hot and cold streams, the energy savings of the hot utility is equal to the energy saving of the cold
             utility and the maximum heat recovered is
                                                                                           (5.6)
                                         q rec ¼ CP h ½TS h  ðTS c þ DT min ފ
                From Eq (5.6), a higher ðDT min Þ results in a smaller (q rec ) and (A ex ) and a higher (q ) and (q ). This

                                                                                 þ
             is well evidenced from Fig. 5.2 as lower overlap (q rec ) of the curves lead to greater extension of the
             curves in the hot and the cold utilities regions.
                Mathematically, the optimal ðDT min Þ is obtained by adding the annual operating cost due to utilities
                               C op, annual over a yearly operating time (t ann ).
                                         C op;annual ¼½C h  ðq h   q rec Þþ C c  ðq c   q rec ފ   t ann  (5.7)
                   Optimal DT min
                               to the annualised investment (C ex ) estimate based on annual interest rate fraction
                               i over the expected lifetime of the plant in years (n ex )

                                                       n ex
                                                                 b ex                      (5.8)
                                                ið1 þ iÞ
                                                     n ex    1
                                         C ex ¼            a ex ½A ex Š
                                               ð1 þ iÞ
                The installed cost of heat exchanger is related to heat transfer area (A ex ) by a power law relation
                                                          b ex                             (5.9)
                                                C ¼ a ex ðA ex Þ
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