Page 452 - Bird R.B. Transport phenomena
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432   Chapter  14  Interphase Transport in Nonisothermal Systems

                                                                            Fig. 14.2-2.  Nusselt numbers
                                                                            for turbulent  flow  of liquid
                                                                            metals in circular tubes,
                                                                            based on the theoretical calcu-
                                                                            lations  of R. H. Notter and
                                                                            C. A. Sleicher, Chem.  Eng, ScL,
                                                                            27,2073-2093(1972).









                               10 2             10 3             10 4
                                         Pe = Peclet number  = RePr



                               It has been  emphasized  that  all the results  of  this  section  are  limited  to fluids  with
                           constant  physical  properties.  When  there  are  large  temperature  differences  in  the  sys-
                           tem,  it  is  necessary  to  take  into  account  the  temperature  dependence  of  the  viscosity,
                           density,  heat  capacity,  and  thermal  conductivity.  Usually  this  is  done  by  means  of  an
                           empiricism—namely, by evaluating the physical properties at some appropriate  average
                           temperature.  Throughout  this  chapter,  unless  explicitly  stated  otherwise,  it  is  under-
                           stood  that  all physical properties  are  to be calculated  at the  film  temperature  T f  defined
                           as  follows: 5
                               a.  For tubes, slits, and other ducts,
                                                                                               (14.2-8)

                                 in which T Oa is the arithmetic average  of the surface temperatures at the two ends,
                                 Ton  =  l(T 0l  +  T 02), and  T ba is  the  arithmetic  average  of  the  inlet  and  outlet  bulk
                                 temperatures, T ba = \{J bl  + T b2).
                                 It  is  also  recommended  that  the  Reynolds  number  be  written  as  Re  =  D(pv)/
                                 IJL  =  DW/S/JL,  in order  to account  for viscosity, velocity, and  density changes  over
                                 the cross section  of area  S.
                               bo  For  submerged objects with  uniform  surface  temperature  T o in  a  stream  of  liquid
                                 approaching with uniform  temperature  T*,,
                                                                Tf = i(T 0 +  To»)             (14.2-9)
                               For  flow systems  involving  more complicated  geometries, it  is preferable  to use ex-
                           perimental  correlations  of  the  heat  transfer  coefficients.  In  the  following  sections  we
                           show how such correlations can be established by a combination  of dimensional  analysis
                           and experimental  data.




                               5
                                W. J. M. Douglas and  S. W. Churchill, Chem. Eng. Prog. Symposium  Series, No. 18, 52, 23-28 (1956);
                           E. R. G. Eckert, Recent Advances  in Heat and Mass Transfer, McGraw-Hill, New  York (1961), pp. 51-81,
                           Eq. (20); more detailed  reference  states have been proposed by W. E. Stewart,  R. Kilgour, and  K.-T. Liu,
                           University  of Wisconsin-Madison  Mathematics  Research Center Report #1310 (June 1973).
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