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Non-equilibrium flow over a wavy wall

Published online by Cambridge University Press:  28 March 2006

Walter G. Vincenti
Affiliation:
Department of Aeronautical Engineering, Stanford University, Stanford, California

Abstract

A small-disturbance solution is obtained for the steady two-dimensional flow over a sinusoidal wall of an inviscid gas in vibrational or chemical non-equilibrium. The results are based on a single, linear, third-order partial differential equation, which plays the same role here as does the Prandtl–Glauert equation in equilibrium flow. The solution is valid throughout the range from subsonic to supersonic speeds and for all values of the rate parameter from equilibrium to frozen flow (in both of which limits it reduces to Ackert's classical solution of the Prandtl–Glauert equation). The results illustrate in simple fashion some of the properties of non-equilibrium flow, such as the occurrence of pressure drag at subsonic speeds and the absence of the discontinuous phenomena that characterize the Prandtl–Glauert theory when the flow changes from subsonic to supersonic.

Type
Research Article
Copyright
© 1959 Cambridge University Press

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References

Ackeret, J. 1928 Über Luftkräfte bei sehr grossen Geschwindigkeiten insbesondere bei ebenen Strömungen. Helv. Phys. acta, 1, 301.Google Scholar
Broer, L. J. F. 1958 Characteristics of the equations of motion of a reacting gas. J. Fluid Mech. 4, 276.Google Scholar
Chu, Boa-Teh 1957 Wave propagation and the method of characteristics in reacting gas mixtures with applications to hypersonic flow. WADC TN-57-213, May 1957.Google Scholar
Gibson, W. E. & Moore, F. K. 1958 Acoustic propagation in a diatomic gas subject to thermal or chemical relaxation. Cornell Aero. Lab. Rep. no. HF-1056-A-2.Google Scholar
Lagerstrom, P. A., Cole, J. D. & Trilling, L. 1949 Problems in the theory of viscous compressible fluids. Calif. Inst. Tech., Report on Contract N6onr-Task Order VII, Office of Naval Research.Google Scholar
Liepmann, H. W. & Roshko, A. 1957 Elements of Gas Dynamics. New York: John Wiley and Sons.
Moore, F. K. 1958 Propagation of weak waves in a dissociated gas. J. Aero Sci. 25, 279.Google Scholar
Moore, F. K. & Gibson, W. E. 1959 Propagation of weak disturbances in a gas subject to relaxation effects. Inst. Aero. Sci. Rep. no. 59-64.Google Scholar
Morrison, J. A. 1956 Wave propagation in rods of Voigt material and visco-elastic materials with three-parameter models. Quart. Appl. Math. 14, 1953.Google Scholar
Wood, W. W. & Kirkwood, J. G. 1957a Characteristic equations for reactive flow. J. Chem. Phys. 27, 596.Google Scholar
Wood, W. W. & Kirkwood, J. G. 1957b Hydrodynamics of a reacting and relaxing fluid. J. Appl. Phys. 28, 395.Google Scholar