Inviscid hypersonic flow around blunt bodies.
Nonequilibrium flow, angles of attack and vapor injection effects on subsonic flow field of blunt body
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Nonequilibrium flow, angles of attack and vapor injection effects on subsonic flow field of blunt body
Optical radiation from wakes of blunt bodies of ablating material measured at hypersonic speeds
Coupling radiative and convective heat transfer in hypersonic blunt body reentry
Blunt bodies stagnation point radiation intensity measurements in supersonic flow at very high stagnation temperatures generated by constricted arc heaters
Time-dependent numerical method for blunt body flow field solutions
Melting ablation for two dimensional and axisymmetric blunt bodies with body force, predicting gas-liquid interface temperature for free stream conditions
Pressure distributions prediction on blunt bodies at angle of attack, considering bodies of revolution and large angle cones
Pressure distributions prediction on blunt bodies at angle of attack, considering bodies of revolution and large angle cones
The viscous, radiating hypersonic flow past an axisymmetric blunt body is analyzed based on the Navier-Stokes equations, plus a radiative equation of transfer derived from the Milne-Eddington differential approximation. The fluid is assumed to be a perfect gas with constant specific heats, a constant Prandtl number of order unity, a viscosity coefficient varying as a power of the temperature, and an absorption coefficient varying as the first power of the density and as a power of the temperature. The gray gas assumption is invoked, thereby making the absorption coefficient independent of the spectral frequency. Limiting forms of the solutions are studied as the freestream Mach number freestream Reynolds number and the temperature ratio across the shock wave, go to infinity, and as the Bouguer number and the density ratio across the shock wave go to zero. The method of matched asymptotic expansions is used in the analysis, and it is shown that there is a far-field precursor, composed of two regions, in which the fluid mechanics can be neglected for all practical purposes but included for completeness.
Accurate semianalytic solutions to the inverse blunt-body problem have been obtained using a method of series expansion. Rational fractions are employed for series summation and analytic continuation. Angles of incidence up to 30 deg and Mach numbers as low as 2 have been considered. The maximum-entropy streamline will not wet the body surface in asymmetric flow. It may pass either above or below the stagnation streamline. Limit lines appear in the supersonic portion of the flow field, both in the shock layer and in its upstream analytic continuation.
A hybridized method for computing the flow about blunt bodies is presented. In this method the flow field is split into its viscid and inviscid parts. The forebody flow field about a parabolic body is computed. For the viscous solution, the Navier-Stokes equations are solved on orthogonal parabolic coordinates using explicit finite differencing. The inviscid flow is determined by using a Moretti type scheme in which the Euler equations are solved, using explicit finite differences, on a nonorthogonal coordinate system which uses the bow shock as an outer boundary. The two solutions are coupled along a common data line and are marched together in time until a converged solution is obtained. Computed results, when compared with experimental and analytical results, indicate the method works well over a wide range of Reynolds numbers and Mach numbers.
The film shows flow over blunt body alone, with internal spike, and with external spikes.
High resolution equilibrium radiation spectra for shock layer of blunt bodies at reentry velocities and radiative recombination of N and O ions
Direct numerical method for calculation of supersonic inviscid flow about axisymmetric blunt body at large angle of attack
Experimental static loads and quasi-steady methods for determining dynamics of separated flow over blunt bodies
Plane and axisymmetric problem of uniform hypersonic flow of viscous gas past blunt bodies
Effect of simulated ablation gas injection on shock layer of blunt bodies at Mach 3 and 5
Nongray self absorption and energy loss effects for blunt body flows during superorbital reentry, considering flow field and wall heat fluxes