Page 442 - Introduction to Continuum Mechanics
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426 Newtonian Viscous Fluid

         6.50. Show that for a one-dimensional, steady, adiabatic flow of an ideal gas, the ratio of
                          at
         temperature #i/#2  sections (1) and (2) is given by






         where y is the ratio of specific heat, MI and MI are local Mach numbers at section 1 and 2
         respectively.
         6.51. Show that for a compressible fluid in isothermal flow with no external work,




         where M is the Mach number. (Assume perfect gas.)
         6.52. Show that for a perfect gas flowing through a constant area duct at constant temperature
         conditions.




         6.53. For the flow of a compressible inviscid fluid around a thin body in a uniform stream of
         speed V m in the Xi - direction, we let the velocity potential be


         where <PI is assumed to be very small. Show that for steady flow the equation governing ^is,
         withM 0 = F 0/c 0
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