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76       BASICS  OF  FLUID  MECHANICS  AND  INTRODUCTION  TO  CFD



                                   z—-kR=(Z-—R)*9(Z),  o(R)  #0,

             a  form  which  avoids  the  sharp  cuspidal  point  and  which,  in  the  vicinity
             of  infinity,  has  the  expansion


                                                     k(k—1)  R?
                                         z=Z4+
                                                          2        Z£
                 In  this  case  the  image  of  acircumference  I  passing  through  —  R  and

             R  will  be  the  union  of  two  circular  arcs,  symmetrical  versus  Og  and
             passing  through  —kR  and  kR.
                 Finally,  if  one  considers  the  image  of  acircumference  I),  passing  only
             through  Z  =  R  and  centered  on  the  OX  axis,  this  image  will  be  tangent
             to  the  previous  symmetrical  contour  at  KR  where  it  has  also  a  sharp  point
             with  the  angle  of  semitangents  equal  to  2km.  Such  an  image  is  known
             as  a  Karman-—Trefftz  profile.  An  application  on  a  dirigible  balloon  of

             Karman—Trefftz  type  is  given  in  chapter  6,  3.3.
                 Writing  the  Joukovski  type  transformation  under  the  form


                                            dz        _(,_B\(,,8
                                           dz              Z)\       TZ}?

             von  Mises  has  considered  the  generalization


                        =  (1-8) (1B)...  (1-H)  kc  am  ek




                 Again  a  circumference  passing  through  Z  =  R  is  transformed  onto  a
              (wing)  profile  of  von  Mises  type,  with  a  sharp  point  at  a  certain  zg  and
             where  the  jump  of  each  semitangent  is  kz.
                 We  remark  that  if  the  Joukovski  type  profiles  depend  on  two  param-
             eters  (like  the  coordinates  of  the  Ty  center),  the  Karman  —  Trefftz  type

             profiles  depend  on  three  parameters  (with  the  additional  k)  while  the
             von  Mises  type  profiles  depend  on  n+  1  parameters.
                JE.  Carafoli  has  introduced  the  transformations  of  the  type  z  =  Z  +
             Ee  +  (Z—byP  with  pa  positive  integer  (the  order  of  the  pole  b).  For  small

             a  one  obtains  quasi—Joukovski  profiles.
                 Caius  Jacob  has  considered  a  class  of profiles  defined  by  the  conformal
             mappings  expressed  in  terms  of  rational  functions  [70].
                 Recently,  I.  Taposu  has  emphasized  a  special  class  of profiles  (“dolphin
             profiles”)  whose  use  in  practice  could  improve  the  classical  concepts  of
             aerodynamics  [139].
                 In  different  laboratories  around  the  world  one  deals  with  classes  of

             profiles  (Naca,  Géttingen,  ONERA,  RAE,  Tzagy,  etc.)  which  are  given,
             in  general,  “by  points”  and,  seldom,  by  their  analytical  form.
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