Page 211 - 48Fundamentals of Compressible Fluid Mechanics
P. 211

10.2. GOVERNING EQUATION                                            173

         can noticed that equations ray:eq:momentum;ray:eq:mass;ray:eq:state are similar
         to the equations that was solved for the shock wave.


                                                                           (10.5)

         The equation of state (10.4) can further assist in obtaining the temperature ratio

         as                                   !



                                                                           (10.6)
                                              !


         The density ratio can be expressed in term of mass conservation as


                          !
                                                                           (10.7)

                          !

                             "



         Substituting equations (10.5) and (10.7) into equation (10.6) yields




                                            "
                                                       !



                                            "
                               "$
                                                                           (10.8)




         Transferring the temperature ratio to left hand side and squaring results in





                                                 !


                                                                           (10.9)



                                                                             and




                                                                      The second

                                 	 %



         law is used to find the expression for derivative.
                                                   *



                The Rayleigh line exhibits two possible maximums one for
                                                                          (10.10)

                    . The second maximum can be expressed as
         for






                                            E
                                 I
                                                                          (10.11)
                                E )	  	 E

                                                                "


         Let the initial condition  , and  are constant then the variable parameters are




           	 , and	 . A derivative of equation (10.11) results in
                                                   E
                     I
                   E


                          " !"
                                                           !"
                                                                          (10.12)


                                           "

                                    #
         Take the derivative of the equation (10.9) when letting the variable parameters be

                                              E


          	 , and 	 results in
                                  I




                                                                          (10.13)


                                                 E



                                 %$'&)( (


                                                      /.
                                       +*-, *  !"
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