Abstract
isochore, isentropic, and isotherm changes of state, respectively. The value of (cn/cp), and hence «, is a function of m*, c* K, 7, andPr. Taking 7= 1.4 and Pr = 0.71, ( c n / c p ) is plotted in Fig. 1 as a function of K. It is shown that depending on m* , c*, and K, ( c n / c p ) can have all of the values corresponding to the above four changes of state or any intermediate values. Now defining a gas stagnation temperature T° ' = T' +u' 1 ( 2 c p ) , it is possible to show from Eqs. (la-c) that x, where
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