Abstract
determined from Eq. (1) and the condition of constant static pressure and total enthalpy. The inviscid flowfield is then calculated from a modified form of Rakich's three-dimensional method of characteristics (NASA TN D-5341). Typical results for the non-dimensional pressure (pb — Pb/p^v^) and inviscid surface Mach Number (Mb) are shown in Fig. 2 for a 20° half-angle cone at a = 10° and Mx = 3. For a velocity defect of A = 0.2 the surface Mach number goes to unity at x = 0.95 (based on B = 10) in the windward plane, and the three-dimensional method of characteristics cannot be continued beyond this point. Member AIAA.
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