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206  HEAT TRANSFER  AND  HEAT  EXCHANGERS
                                                                   7.  Continue with other specifications of  the vapor temperature  T,,
                                                                      one interval at a time,  until  the required  outlet temperature is
                                                                      reached.
                m                                   I   Coolant phase   8.  The heat transfer area will be found by numerical integration of
                  Gas phase
                                                                                                               (8.39)
                                                       TL
                                                                   Examples  of  numerical  applications  of  this  method  are  in  the
                                                                    original paper of  Colburn and Hougen (1934), in the book of  Kern
                                                                    (1950, p. 346) and in the book of  Ludwig (1983, Vol. 3, p.  116).

                  Interlace   -                                     The Silver-Bell-Ghaly   Method
                   PI  8  T,                                       This method takes advantage of  the rough proportionality between
                                                                    heat  and  mass  transfer  coefficients  according  to  the  Chilton-
                Figure  8.15.  Model  for  partial  condensation  in  the  presence  of   Colburn analogy, and employs only heat transfer coefficients for the
                uncondensed  material:  U(T - TL) = hg(Tg - T) + Akg(p, -pi).   process of  condensation from a mixture. The sensible heat  Q,  of
                [A.P. Colburn and  O.A. Hougen, Ind.  Eng.  Chem. 26, 1178-1182   the vapor is transferred through the gas film
                (1 934)J
                                                                       dQ,  = h,(T,  - Ti) dA.                  (8.40)
                8.12.  The  calculation of  condensation  of  pure  vapors  is  straight-   In  terms  of  an  overall  heat  transfer  coefficient U  that  does  not
                forward.  That  of  mixtures  occurs  over  a  range  of  temperatures   include the  gas film, the total  heat  transfer QT that  is made up of
                and involves mass transfer resistance through  a gas film  as well as   the  latent  heat  and  the sensible heats  of  both  vapor and  liquid is
                heat transfer resistance by liquid and fouling films. A model due to   represented by
                Colburn  and  Hougen  (1934)  is  represented  by  Figure  8.15.  The
                overall rate of  heat  transfer is regarded as the  sum of  the sensible   dQT = U(q - TL) dA.   (8.41)
                heat transfer through a gas film and the heat of  condensation of  the
                material transferred by diffusion from the gas phase to the interface.   When the unknown interfacial temperature   is eliminated and the
                The  equation  of  this  heat  balance  is,  in  terms  of  the  notation  of   ratio Z of  sensible and total heat transfers
                Figure 8.15,
                   u(T - TL) = hg(Tg - I;) + akg(pg -pi).   (8.37)
                                                                    is introduced, the result is
                The temperature TL of  the coolant is related to the heat transfer Q
                by
                                                                                                                (8.43)
                   dQ = mLCL dT,

                or the integrated form                              which is solved for the heat transfer area as

                   TL = TLo + AQlmLCL.                      (8.38)                                              (8.44)
                A procedure will be  described for taking the vapor from its initial
                dewpoint  Tgo to  its  final  dewpoint corresponding to  the  required   Since  the  heat  ratio  Z,  the  temperatures  and  the  heat  transfer
                amount  of  condensation.  Gas  temperatures  are  specified  at   coefficients vary  with  the  amount  of  heat  transfer  QT up  to  a
                intermediate  points  and  the  heat  balance  is  applied  over  one   position  in  the  condenser,  integration  must  be  done  numerically.
                interval at a time.                                 The  coolant  temperature  is  evaluated  from  Eq.  (8.38).  Bell  and
                                                                    Ghaly (1973) examine cases with multiple tube passes.
                1. Prepare the condensing curve, a plot of the vapor temperature T,   The  basis  of  the  method  was  stated  by  Silver  (1947).  A
                  against the amount of  heat removed Q, by a series of isothermal   numerical  solution  of  a  condenser  for  mixed  hydrocarbons  was
                  flashes and enthalpy balances.                    carried  out  by  Webb  and  McNaught  (in  Chisholm, 1980, p.  98);
                2.  Starting at the inlet temperature  Tgo, specify a temperature T, a   comparison  of  the  Silver-Bell-Ghaly  result  with  a  Colburn-
                  few degrees less, and note the heat transfer AQ corresponding to   Hougen calculation showed close agreement in this case. Bell and
                  this temperature  difference from the condensing curve.   Ghaly (1973) claim only that their method predicts values from 0 to
                3. Find the temperature TL of  the coolant with Eq. (8.38).   100% over the correct values, always conservative. A solution with
                4.  Assume an interfacial temperature T, then find the correspond-   constant  heat  transfer  coefficients is  made  in  Example  8.11:  A
                  ing vapor pressure pi and latent heat A.          recent  review of  the  subject has been  presented by  McNaught (in
                5.  From available correlations, find values of  the coefficients h,,  k,,   Taborek et al.,  1983, p. 35).
                  and  U which  are  temperature-  and  composition-dependent,
                  although they  sometimes may be  taken  as  constant  over some
                  ranges.                                           8.9.  REBOILERS
                6.  Check if  these values satisfy the heat  balance of  Eq.  (8.37). If   Reboilers  are  heat  exchangers that  are  used  primarily to provide
                  not,  repeat  the  process  with  other  estimates of  I;. until  one is   boilup for distillation and similar towers. All types perform partial
                  found that does satisfy the heat balance.         vaporization of  a stream flowing under natural or forced circulation
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