Page 191 - Chemical process engineering design and economics
P. 191

Process Heat Transfer                                           173


                Use Equations 4.4.13 and 4.4.3 to  eliminate m  and A from  the total cost
                                                      li W  0
            equation, Equation 4.4.6. Thus,

                   Q 6 C w     Q (C c + CM)
            C T=————————     +  ———————                                 (4.4.14)
                CPW (t 2,w -  ti. w)  U 0 F (At) LM

                 With the exception of F, all the parameters in both terms in Equation 4.4.14
            are constants.  In  order to obtain a first  approximation for the exit-water tempera-
            ture  and  to  simplify  the  derivation,  assume  that  F  is  constant.  To  obtain an  eco-
            nomically-viable heat exchanger, let F = 0.85.
                 After  substituting  the  logarithmic-mean  temperature  difference,  Equation
            4.4.4, into Equation 4.4.14 we find that



                 FQ9C W                Q(C C + C M)         (t4,p-t llW)
               =  —————————   +  ——————————————————       In  ——————   (4.4.15)
            C T
                 Cpw (t 2,W - ti,w)  U 0 F [ (t4 jP - ti\n) - (taj
                Equation 4.4.15 can now be  differentiated  with respect to t,w  After  setting
                                                               2
            the derivative equal to zero, and rearranging the equation, it is found that
                U 0 6 C w (A^ -  At 2) 2  (At!-At 2)
                                                                       (4.4.16)
             Cp W(C F + C M)  (t 2,w-ti,w) 2  At 2  At 2

            where At t  = t^f  -  t\\N and At 2 = ts ;p -  t 2jw  Equation 4.4.16 is dimensionless. The
                                           t
            optimum  cooling-water  temperature, ,  is  obtained  from  Equation  4.4.16  by
                                           2;W
            iteration.




            APPROACH TEMPERATURE DIFFERENCES

            Frequently, an approximate value of the optimum exit-water temperature is all that
            is required, and a rule-of-thumb  will be  satisfactory.  Table 4.4 lists the  approach
            temperature difference,  which is the difference  between the two terminal tempera-
            tures  of two passing  streams,  for several heat  exchangers.  Several approach tem-
            perature differences  were taken from Ulrich [8].  For refrigerants, Ulrich's range of
            10 to 50°C is on the high side.  Frank [7] recommends a range of 3 to 5°C whereas
            Walas [3] recommends a value of 5.6°C or less.





         Copyright © 2003 by Taylor & Francis Group LLC
   186   187   188   189   190   191   192   193   194   195   196