Turbulent, viscous interaction theory is used to understand the hypersonic flow past an expansion corner. By assuming a pressure law, the boundary-layer properties of the flow are obtained through simultaneous solution of a displacement thickness relationship and a coupling equation relating the effects of incidence and displacement thickness to the effective body shape. The pressure law is obtained through examination of available experimental data. The form of the pressure law is found to depend on the incidence. The pressure decay is dependent on both viscous and incidence effects. For weak incidence, viscous effects are important throughout the interaction, and they produce a gentle pressure decay. For strong incidence, viscous effects are important only near the front of the corner. In this latter case, the pressure decays rapidly followed by a long asymptotic downstream region; the overall pressure distribution then appears more similar to the in viscid case.
NomenclatureA B C^ = constant of proportionality in linear viscosity-temperature relationship K -hypersonic similarity parameter, M^cc K v = modified hypersonic similarity parameter, M^ dy e (x)/ dx M = Mach number P(x) = nondimensional pressure, p^/pp = pressure Re = unit Reynolds number T = temperature U = velocity (x, y) = physical coordinates along and normal to the incoming flow a = expansion corner angle y = ratio of specific heats 8 = boundary-layer thickness 6* = boundary-layer displacement thicknesŝ = dummy variable of integration p = density % = weak turbulent, viscous interaction parameter, (M 9 C / Re*) 115 Subscripts e = edge condition or effective w = wall condition oo = incoming freestream condition 0 -stagnation condition