Asymptotic Solutions at the Moving Shock Front

Matching of Asymptotic Solutions at the Moving Shock Front 

It follows from this equation that %(0 0, at t Unknown functions Ofq) and F(q) obey the following equations  

After integration of Equation A5.2 and Equation A5.3 with boundary conditions F 1, 0 0, at °o, we get 

Equation A5.10 shows that boundary conditions (5.166) at the shock front are the only possible conditions that can be matched with the inner solution. From the above derivation we conclude that in the boundary layer 

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Matching of asymptotic solutions at the moving shock front. 

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