Titlebook: Shock Waves @ Marseille I; Hypersonics, Shock T Raymond Brun,Lucien Z. Dumitrescu Conference proceedings 1995 Springer-Verlag Berlin Heidel

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DRILL

Effects of Leading-Edge Bluntness on Control Flap Effectiveness at Hypersonic Speedsin a hypersonic gun tunnel facility at .. = 8.2 and ../. = 9.0 × 10.. The flow structure over a low aspect ratio flat plate with a full span trailing edge flap has been investigated using high speed Schlieren photography as well as surface pressure and heat transfer measurements.

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Measuring the Effect of Nose Bluntness on Drag of a Cone in a Hypervelocity Shock Tunnel Facilitynd hypervelocity (flight speed & 5 km/s) regime. Experiments were performed in a free-piston driver shock tunnel facility. Drag measurements were made using the de convolution force balance (Sanderson and Simmons 1991) for measuring drag in hypervelocity impulse facilities where test times may be of

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IVORY

Oblique Shock Interactions with Mach Number Distributions-Hugoniot shock jump conditions. This equation essentially describes the shape an oblique shock assumes as it traverses a region of varying Mach number. Because the analysis also provides a flow solution downstream of the shock, it is seen as a particularly useful tool in the study of shock wave — m

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Strength of Characteristics at a Curved Shock Wavee gradient and streamline curvature are used to determine the relative strengths (the reflection coefficient) of characteristics just downstream of a two-dimensional curved shock wave. It is shown that the characteristics’ strengths are a complex function of the specific heat ratio, the upstream Mac

Enthralling

Blunt Body Flow — The Transonic Regionthe downstream surface of the shock wave and the limiting characteristics. Using curved shock theory, we establish the conditions under which the shock surface is (type I), or is not (type II), a boundary of the transonic region. It is found that the existence of type I or type II flow is determined