Boundary Condition at the Moving Shock Front

Derivation of Boundary Condition at the Moving Shock Front 

Multiplication of Equation 5.156 and Equation 5.157 by r and integration over r from to where r it) rj, where r r2 are some constant values, yields 

Where we use the following abbreviation f, = f(r). The left-hand side of Equation A4.1 and Equation A4.2 can be transformed in the following way  

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Derivation of boundary condition at the moving shock front. 

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