Page 463 - Bird R.B. Transport phenomena
P. 463

§14.6  Heat Transfer  Coefficients  for  Free and Mixed Convection  443

                                It  has  been  shown,  however,  that  simple  and  reliable  predictions  of  heat  transfer
                            rates (expressed  as area mean Nusselt numbers Nu ) may be obtained for  this wide  vari-
                                                                       m
                            ety  of  flow  regimes  by  empirical combinations  of asymptotic  expressions:
                                a.  Ni4  ond , for  conduction in the absence  of buoyant  forces  or forced  convection
                                b.  Nujj , for  thin laminar boundary  layers, as in Example  11.4-5
                                      m
                                      rb
                                с  Nu^ ,  for  turbulent boundary  layers
                                d.  Nu^  rced /  for  pure forced  convection
                            These are dealt with  in the following  subsections.

       No Buoyant Forces
                            The  limiting  Nusselt  number  for  vanishingly  small  free  and  forced  convection  is  ob-
                                                                                         2
                            tained by  solving the heat conduction equation (the Laplace equation, V T  =  0) for  con-
                            stant, uniform temperature over the solid  surface  and a different  constant temperature at
                            infinity.  The mean Nusselt number then has the general  form
                                                          Nu c ond  = K(shape)                  (14.6-2)
                                                             m
                            With  К equal  to zero  for  all  objects  with  at  least  one infinite  dimension  (e.g.,  infinitely
                            long cylinders  or infinitely  wide  plates). For finite bodies  К is nonzero, and an important
                            case is that of the sphere for  which, according to Problem 10B.1,
                                                             Nu™ nd  = 2                        (14.6-3)
                            with  the characteristic length  taken to be  the sphere diameter. Oblate ellipsoids  of  revo-
                            lution and circular disks  are discussed  in Problem 14D.1.

       Thin Laminar Boundary    Layers

                            For  thin  laminar  boundary  layers,  the  isothermal  vertical  flat  plate  is  a  representative
                            system,  conforming  to Eq. 14.6-1. This equation may be generalized  to
                                                     NujT  = C(Pr, shape)(GrPr) 1/4              (14.6-4)

                            Moreover, the function  of  Pr and shape can be factored  into the product
                                                       С  = C (shape)C (Pr)                      (14.6-5)
                                                            1
                                                                    2
                            with 2
                                                                 0.671                          (14.6-6)
                                                                          l
                                                               (0.492/Pr) 9/16 |4/9
                                              1 3
                            Representative values '  of  Q  and C  are given  in Tables  14.6-1 and  2, respectively.  Shape
                                                          2
                                                                           3 4
                            factors  for  a wide  variety  of  other shapes  are available. '  For heated  horizontal  flat  sur-
                            faces  facing  downward  and cooled horizontal flat surfaces  facing  upward, the  following
                                     5
                            correlation  is recommended:
                                                               ° ^        (GrPr)  1/5            (14.6-7)
                                                             (1.9/Pr) 9/10 ]  2


                                2
                                 S. W. Churchill and  R. Usagi, AlChE  Journal, 23,1121-1128 (1972).
                                3
                                 W.  E. Stewart, Int. J. Heat and Mass  Transfer, 14,1013-1031  (1971).
                                4
                                 A. Acrivos,  AIChE  Journal, 6, 584-590  (1960).
                                 T. Fujii, M. Honda, and  I. Morioka, Int. J. Heat and Mass  Transfer, 15, 755-767  (1972).
                                5
   458   459   460   461   462   463   464   465   466   467   468