Page 116 - Aeronautical Engineer Data Book
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92      Aeronautical Engineer’s Data Book
                            2
        Momentum  p + p u = p +   u  2
                                    2 2
                                2
                          1 1
                      1
                         2          2
                        u 1        u 2
        Energy  c T +   = c T +   = c T    0
                             p
                    1
                  p
                                2
                                         p
                        2           2
      Pressure and density relationships across the
      shock are given by the Rankine-Hugoniot
      equations:
                + 1
                    2
                    – 1
         p  2
                –1   1
            =

                + 1
                 –
         p  1          2
                 –1    1
              (  + 1)p 2
                + 1
           2  (  –1)p 1
            =
                      p
                 + 1
           1      +
                       2
                 –1  p 1
      Static pressure ratio across the shock is given
      by:
                  2
              2  M – (  – 1)
         p 1      2
           =
                    + 1
         p 2
      Temperature ratio across the shock is given by:
         T 2  p 2   2
           =
         T 1   p /   1
               1
                                         2  �
             �
                             ��
                    2
                                           2
                               2 + (  – 1)M
               2  M – (  + 1)
         T 2
                                           1
                    1
           =
         T 1         + 1         (  + 1)M 1
      Velocity ratio across the shock is given by:
        From continuity:  u 2 /u 1 =   1 /  2
                             2 + (  – 1)M 2
                        u 2             1
        so:               =
                        u 1    (  + 1)M 2
                                       1
      In axisymmetric flow the variables are indepen­
      dent of     so the continuity equation can be
      expressed as:
               2
         1  ∂(R q )      1    ∂(sin  q )
                  R

             +      = 0
         R 2   ∂R     R sin      ∂
      Similarly in terms of stream function  :
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