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11.6  Model  Problem:  Laminar  and  Turbulent  Flat  Plate  Flow     343



         -  The top boundary  velocities are specified  and the pressure  is extrapolated;
         -  The bottom  boundary  is  specified  on the  flat  plate,  with  zero  pressure-
            gradient  normal  to the wall.  Symmetric  flow  is specified  upstream  of the
            plate;
         -  The left  boundary  conditions  are specified,  and the normal  velocity  is  ex-
            trapolated  from  the interior;
         -  The  right  boundary  pressure is specified,  and the  velocities  are  extrapolated.
            The  resulting  program  is  included  in Appendix  B.  Since  the changes are
         minimal, the program  is not  further  discussed  here, except that  for  commonality,
         the  eddy  viscosity  is computed  for both  laminar  and turbulent  flows.  In the
         former,  the values  are set to zero,  whereas  in the latter,  they  are  obtained  with
         the  Cebeci-Smith  turbulence  model.
            Figure  11.4  shows  the results  for a  laminar  flow  at  a  Reynolds  number  of
           6
         10 .  Figure  11.4a  shows  the velocity  profiles  at two x-stations  together  with
         the  Blasius  solution  [16], and Fig.  11.4b  shows the computed  local  skin-friction
         results  with the Blasius  solution.




                                                                    Blflsais
                                                                    INS2D
                       Qu»rticRx=  0.50 10*       a
                       QUBrticRX-  0.80 10 '   *   0  005
                       INS2D  flx=  0.50  10*
                       IN92D  R x ,  0.80 10 c   -•
                                              0004   7«
                                     •  A
                                              0  003 _  i
                                  •   M.




            ^
                           u/U
         (a)                                 (b)
         Fig.  11.4.  Comparison  of computed  and Blasius  results  for a laminar  flow at a  Reynolds
                   6
         number  of 10 . (a) velocity  profiles  and (b) local  skin-friction  coefficients.


            The  computed  results  for a  turbulent  flow  over  a  flat  plate  at  a  Reynolds
                      7
         number  of 10  are shown  in Figs.  11.5  and 11.6  together  with  the empirical
         relations  based  on experimental  data  [16].  Figure  11.5a  shows  a  comparison
                                                                   l
         between  the  computed  velocity  profiles  and  those  based on the / 7  t h  power-law
         profile  [16] and Fig.  11.5b  shows  those  for the local  skin-friction  coefficients.
            In  order  to  validate  the turbulence  model  implementation,  the  near-wall
         region  is examined  further  in Fig.  11.6. As can be seen, the Cebeci-Smith  tur-
         bulence  model  duplicates  the experimentally  observed  laminar  sublayer and
         law-of-the  wall  region.
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