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References                                                            261



         8.5.3  Transition  Prediction  for  Airfoil  Flow

         The  procedure  for  determining  the  onset  of  transition  location  on  an  airfoil  is
         similar  to  the  procedure  used  for  the  flat  plate  flow  discussed  in  the  previous
         subsection.  To demonstrate  this,  we consider  an NACA  0012 airfoil  at  two  chord
                                             6
         Reynolds  numbers,  R c  =  10 6  and  3 x  10 .  For  the  external  velocity  distribution
         obtained  from  the  HSPM  computer  program  discussed  in  Section  6.5, the  lami-
         nar  velocity  profiles  are computed  with  BLP  for  a  =  0°,  2°  and  4°. The  neutral
         stability  calculations  are then  performed  for  each  Reynolds number  and  angle  of
         attack.  These  calculations  were then  followed  by  amplification  rate  calculations
         for  each  frequency  computed  on  the  neutral  stability  curve.  For  each  calcula-
         tion,  the  transition  location  is determined  with  respect  to  the  surface  distance
         along  the  perimeter  of  the  airfoil  measured  from  the  stagnation  point  and  the
         corresponding  x/c  location  is  calculated.
            Table  8.2  presents  a summary  of the  calculated  transition  locations  at  three
         angles  of  attack  and  two  chord  Reynolds  numbers  for  n  — 8.  The  results  show
         that  with  increasing  angle  of attack,  since the adverse pressure gradient  becomes
         stronger,  the  transition  location  moves  upstream.  The  results  also  show  that
         with  increasing  Reynolds  number,  the  transition  location  moves  upstream.

         Table  8.2.  Onset  of transition  locations  on the  upper  surface  of  an
         NACA  0012  airfoil  at  two  Reynolds  numbers  and  three  angles  of
        attack.
        a           0°             2°              4°

         Rc         (s/c)tr-(x/c)tr  (s / c)tr~(x  / c)tr  (s /' c) tr~(x  /' 6)  tr
         1  x  10 6  0.505-0.49    0.33-0.31       0.16-0.13
         3  x  10 6  0.355-0.34    0.21-0.19       0.10-0.075



           More applications  of STP,  including  its extension  to three-dimensional  flows
        can  be  found  in  [3].


         References

         [1]  Kleiser,  L.  and  Zong,  T.A.:  "Numerical  Simulation  of  Transition  in  Wall  Bounded
            Shear  Flows,"  Annual  Review  of  Fluid  Mechanics,  Vol.  23, pp.  495-538,  1991.
         [2]  Herbert,  T.:  "Parabolized  Stability  Equations,"  Special  Course  on  Progress  in  Tran-
            sition  Modeling,  AGARD  Report  793, April  1994.
         [3]  Cebeci,  T.:  Stability  and  Transition:  Theory  and  Application,  Horizons  Pub.,  Long
            Beach,  Calif,  and  Springer,  Heidelberg,  2004.
         [4]  Smith,  A.M.O.:  "Transition,  Pressure  Gradient,  and  Stability  Theory,"  Proceedings
            IX  International  Congress  of  Applied  Mechanics,  Brussels,  Vol.  4, pp.  234-2  4,  1956.
         [5]  Van  Ingen,  J.L.:  "A  Suggested  Semi-empirical  Method  for  the  Calculation  of  the
            Boundary-Layer  Region,"  Report  No. VTH71,  VTH74,  Delft,  Holland,  1956.
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