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200                          6.  Inviscid  Flow  Equations  for  Incompressible  Flows


           0.00  n




          -0.02+

          -0.03 +

          -0.04+

          -0.05-1    H    1   1   1   I      -I  1-
              0   2   4   6   8  10  12  14  16  1B  20
                                 a
         Fig.  6.11.  Variation  of  the  moment  coefficient  c m  with  angle  of  attack,  a  for  the  NACA
         0012  airfoil.
























         Fig.  6.12.  Distribution  of  the  pressure  coefficients  around  a  circular  cylinder  for  four
         values  of  7.


         revised  computer  program  and  contains the  modifications  required  to  each  sub-
         routine  (except  GAUSS  and  CLCM)  of  the  panel  program  and  to  its  MAIN
         program.
            Figure  6.12  shows  the  computed  pressure  coefficients  around  the  circular
         cylinder  for  values  of  r  (GAMMA)  equal  to  0,  1,  2 and  3.  These  results  are  in
         excellent  agreement  with  the  analytical  solution  with

                                   v                r                       (6.6.3)
                                  —   =  2 s i n 0 +  —
                                                    r
                                  Voo            27rV 00ro
         obtained  from  inviscid  flow  theory  as  described,  for  example,  in  Anderson  [2].
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