The usefulness of the shock-layer approximation is studied as a method of attacking hypersonic gasdynamics of a blunt body. This paper is concerned mainly with the inverse problems of axisymmetric inviscid flow of a calorically perfect gas (in which the shock geometry is given). Methods that are consistent with approximations based on a high- shock- compression ratio (but modified for the contribution of the tangential pressure gradient and some other second-order terms) are proposed. Agreement in body shape and streamlines with other more exact (numerical) solutions is shown not only for specific heat ratios (as high as y = 2), but also for stagnation regions of very blunt configurations (for which the standard shock-layer theory completely fails). Analytic forms of the pressure field, body, and streamline geometries are developed for the conic-family shocks (of arbitrary degree of oblateness and eccentricity) in the stagnation regions. Nomenclature 6 = a length scale characterizing the subsonic region Bs = oblateness parameter for the conic section shock, Eq. (26) Hm, Ifco, Um = free-stream stagnation enthalpy, freestream Mach number, and free-stream velocity, respectively N, n = eMoc.2 and (Ar — 1)/2(N + 1), respectively p, p, u, v = pressure, density, velocity components parallel to x and y, respectively p, p, ii, v = p} p, u, and v nondimensionalized by Poof^co 2, Poo/e', Um and e'f/oo, respectively pj p, u, v = dimerisionless perturbation pressure, perturbation density, tangential velocity, and normal velocity, respectively, in the stagnation region, defined in Eq. (17) Q(rt r#)t R(r, r#) = functions defined in Eq. (8) r =
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