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180  HEAT TRANSFER  AND  HEAT  EXCHANGERS



                    EXAMPLE 8.4                                      tabulation:
                    Performance of a Heat Exchanger with the F-Method
                 Operation  of  an  exchanger is  represented  by  the  sketch  and  the   T   P   R   (An,,,,   F   G
                 equation                                                     145.0  0.458 1.375  72.24  0.679  0.94
                                                                              145.197 0.457 1.370  72.35 0.691   0.00061
                    Q/UA = 50 = F(AT),,                                       145.5  0.454 1.363  72.51  0.708 -1.34
                                                                        le  !  Examp le 8.4.  The  F-niett-rod
                                                                        .-. -
                                                                        rlLt  SHORT  P c  R >  F .*  T 1
                                                                        38 INPIJT  T
                                                                        .) "1  P= < 20a-T > ~'120
                                                                        50 R=<28@-TjH4#
                                                                        68 TI=( T-  16Bj.~LllI;( (T-Y#)/8@)
                             Ll_tz 2oo 120                              7EI  E=<R"..2+1 jA.5
                                                                        :3 8 F=E,(R-l   :!SLOG< < l-Pj,*c  l-PSR>)
                                                                        sa  F=Fx'LOG < < 2-PB  <R+ 1-E  3 1,  (Z-PXI
                 The outlet temperature of  the hot fluid is unknown and designated   R + 1 +E  2 >
                                                                                   :J
                 by  T. These quantities are formulated as follows:     35  G=5@-F$T1
                                                                       188  PRIHT  "T=" i T
                        p=-  200 - T                                   110  PRINT  "I;=" j G
                           200 - 80 '                                  120  PRINT  "P=" ; P
                        Rs-  200-  T                                   130  PRINT  "R="  ;R
                           120-80'                                     140  PRINT  "F=".;F
                                                                                     I' T 1 =I1  ; T 1
                                                                       158  PI?: I t4T
                            T - 80 - (200 - 120)                       168  GOTO  3B
                    (AT)lm=ln[(T  - 80)/(200 - 120)]                   170  EblD
                 F  is  represented  by  the  equation  of  Item  6  of  Table  8.3,  or  by
                 Figure 8.4(a). Values of  T are tried until one is found that satisfies   T=  145.197
                 G = 50 - F(AT),, = 0. The printout shows that         I;=   ,88249286
                                                                       P=  .45669
                     T = 145.197.                                      R=  1.3701
                                                                       F=  ,69189
                 The  sensitivity  of  the  calculation  is  shown  in  the  following   Tl=  72.346





                 physical  properties  and  operating  conditions.  The  reliabilities of   maintained in  a  particular plant  is  not  certain.  Sometimes fouling
                  these classes of  data increase in the order of this listing, but also the   develops slowly; in  other  cases it  develops quickly as  a  result  of
                  ease of  use of  the data diminishes in the same sequence.   process  upset  and  may  level  off.  A  high  coefficient  often  is
                                                                     desirable,  but  sometimes is  harmful  in  that  excessive subcooling
                  OVERALL COEFFICIENTS                               may occur or film boiling may develop. The most complete list of
                                                                     fouling factors  with  some  degree  of  general  acceptance is  in  the
                  The  range  of  overall  heat  transfer  coefficients is  approximately   TEMA  (1978)  standards.  The  applicability of  these  data  to  any
                  10-200 Btu/(hr)(sqft)("F).  Several  compilations  of  data  are   particular  situation,  however,  is  questionable  and  the  values
                  available, notably in the  Chemical Engineers Handbook  (McGraw-   probably  not  better  than  *50%.  Moreover,  the  magnitudes and
                  Hill, New York, 1984, pp.  10.41-10.46)  and in Ludwig (1983, pp.   uncertainties of  arbitrary fouling factors may take the edge off  the
                  70-73).  Table 8.4 qualifies each listing to some extent, with respect   importance  of  precise calculations of  heat  transfer  coefficients. A
                  to the kind of  heat transfer, the kind of equipment, kind of  process   brief discussion of fouling is by Walker (1982). A symposium on this
                  stream,  and temperature range. Even so, the range of  values of  U   important topic is edited by Somerscales and Knudsen (1981).
                  usually  is  two-  to  three-fold,  and  consequently  only  a  rough
                  measure of equipment size can be obtained in many cases with such   INDIVIDUAL FILM COEFFICIENTS
                  data.  Ranges of  the coefficients in various kinds of  equipment are
                  compared in Table 8.5.                             Combining individual film coefficients into an overall coefficient of
                                                                     heat transfer allows taking into account a greater variety and range
                  FOULING FACTORS                                    of  conditions, and should provide a better estimate. Such individual
                                                                     coefficients are listed in Tables 8.6 and 8.7. The first of  these is a
                  Heat  transfer  may be  degraded  in  time  by  corrosion,  deposits of   very  cautious  compilation  with  a  value  range  of  1.5-  to  2-fold.
                  reaction products, organic growths, etc. These effects are accounted   Values of  the fouling factors are included in the coefficient listings
                  for  quantitatively  by  fouling  resistances,  l/hf.  They  are  listed   of  both tables but are not identified in Table 8.7. For clean service,
                  separately in Tables 8.4 and 8.6, but the listed values of  coefficients   for example, involving sensible heat transfer from a medium organic
                  include these resistances. For instance, with a clean surface the first   to heating a heavy organic,
                  listed value of U in Table 8.4 would correspond to a clean value of
                  U = 1/(1/12 - 0.04) = 23.1.  How  long  a  clean  value  could  be   U = 10,000/(57 - 16 + 50 - 34) = 175
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