Page 85 - Mechanical Engineers' Handbook (Volume 4)
P. 85

74   Fluid Mechanics













                                                                Figure 26 Mach numbers across a normal
                                                                shock, k   1.4.

                                                             1
                                              y    k   1  p y      p y     k   1
                                              x    k   1 p x       p x  k   1
                          and is plotted in Fig. 27, which shows that weak shocks are nearly isentropic, and that the
                          density ratio approaches a limit of 6 for gases with k   1.4.
                             Gas tables show that at an upstream Mach number of 2 for air, M   0.577, the pressure
                                                                                y
                          ratio is p /p   4.50, the density ratio is   /    2.66, the temperature ratio is T /T   1.68,
                                                                                           x
                                                                                        y
                                                          y
                                                             x
                                   x
                                 y
                          and the stagnation pressure ratio is p /p 0x    0.72, which indicates an entropy increase of
                                                       0y
                          s   s   R ln(p /p )   94 J/kg.
                          y
                                        0y
                              x
                                            0x
           10.4  Oblique Shocks
                          Oblique shocks are inclined from a direction normal to the approaching streamlines. Figure
                          28 shows that the normal velocity components are related by the normal shock relations.
                          From a momentum analysis, the tangential velocity components are unchanged through























                                                Figure 27 Rankine–Hugoniot curve, k   1.4.
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