Page 310 - Bird R.B. Transport phenomena
P. 310

294  Chapter 10  Shell Energy  Balances and Temperature Distributions in Solids and Laminar Flow

                               Once  the  temperature and  heat  flux  distributions  are  known,  various  information
                           about the system  may be obtained:

                               (i)  Maximum  temperature rise (at r  = 0)

                                                         T  m a x  -  T o  = ^                 (10.2-14)

                               (ii)  Average temperature rise
                                                         27Г  [R
                                                                   -  т

                                                              2    rdrdO
                                                            Jo

                           Thus the temperature rise, averaged  over  the cross  section, is  half  the maximum temper-
                           ature  rise.
                               (iii)  Heat outflow at the surface  (for  a length  L of  wire)

                                             Q\ r=R  =  lirRL  •  q \ =R =  2irRL  ш ^ п  =  irRl L  ' e  (10.2-16)
                                                                                  S
                                                                              '
                                                            r r
                           This result  is not surprising,  since, at steady  state, all the heat produced by  electrical  dis-
                                                 2
                           sipation in the volume  TTR L must leave  through the surface  r  = R.
                               The reader, while  going  through this development, may well have had the feeling  of
                           deja vu. There is, after  all, a pronounced similarity  between  the heated wire  problem and
                           the viscous  flow  in a circular tube. Only the notation is  different:


                                                       Tube   flow   Heated wire
                           First integration gives
                           Second integration gives   v (r)         T(r) -Т„
                                                      z
                           Boundary condition at r = 0  T  =  finite    finite
                                                       rz
                           Boundary condition at r = R  v  = 0      T-    -  U
                                                      z                 i 0
                           Transport property                       k
                           Source term                (%  -  9> )/L  Se
                                                            L
                           Assumptions                /л = constant  k,k = constant
                                                                      e
                           That  is,  when  the  quantities  are  properly  chosen,  the  differential  equations  and  the
                           boundary  conditions  for  the two  problems  are identical, and  the physical  processes  are
                           said  to be  "analogous."  Not all problems  in momentum transfer  have  analogs  in  energy
                           and mass  transport. However,  when  such analogies  can be  found, they may be useful  in
                           taking  over  known  results  from  one  field  and  applying  them  in  another. For  example,
                           the  reader  should  have  no  trouble  in  finding  a  heat  conduction analog  for  the  viscous
                           flow in a liquid  film  on an inclined plane.
                               There  are  many  examples  of  heat  conduction problems  in  the  electrical  industry. 1
                           The minimizing  of temperature rises  inside  electrical machinery prolongs  insulation  life.
                           One  example  is  the  use  of  internally  liquid-cooled  stator  conductors  in  very  large
                           (500,000 kw)  AC generators.




                               1  M. Jakob, Heat Transfer, Vol.  1, Wiley, New York  (1949), Chapter 10, pp. 167-199.
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