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A multiple-scales model of the shock-cell structure of imperfectly expanded supersonic jets

Published online by Cambridge University Press:  20 April 2006

Christopher K. W. Tam
Affiliation:
Department of Mathematics, Florida State University, Tallahassee. Florida 32306
Jay A. Jackson
Affiliation:
Department of Mathematics, Florida State University, Tallahassee. Florida 32306
J. M. Seiner
Affiliation:
NASA Langley Research Center, Hampton, Virginia 23365

Abstract

A linear solution modelling the shock-cell structure of an axisymmetric supersonic jet operated at slightly off-design conditions is developed by the method of multiple scales. The model solution takes into account the gradual spatial change of the mean flow in the downstream direction. Turbulence in the mixing layer of the jet has the tendency to smooth out the sharp velocity and density gradients induced by the shocks. To simulate this effect, eddy-viscosity terms are incorporated in the model. Extensive comparisons between the numerical results of the present model and experimental measurements gathered at the NASA Langley Research Center over the Mach number range of |Mj2Md2| [les ] 1.0 for underexpanded and overexpanded supersonic jets are carried out. Here Mj is the fully expanded jet Mach number and Md is the design Mach number of the convergent–divergent nozzle. Very favourable agreement is found. This is especially true for the gross features of the shock cells, including the shock-cell spacings and the pressure amplitudes associated with the shocks. The measured data show that the pressure distributions over the first three or four shock cells usually are rich in fine structures. These fine structures are reproduced by the calculated results. Beyond the first few shock cells the model predicts that the shock-cell structure can be represented by a single Fourier mode of the mean flow. This is confirmed by a careful examination of the experimental data. The appropriate turbulent Reynolds number for shock-cell structure calculation is investigated. It is shown that the best choice is the same as the value found to give the best results for jet mean-flow calculation. The present model is used to explain some of the observed characteristics of broadband shock-associated noise.

Type
Research Article
Copyright
© 1985 Cambridge University Press

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References

Adamson, T. C. & Nicholls, J. A. 1959 On the structure of jets from highly underexpanded nozzles into still air. J. Aero. Sci. 26, 1624.Google Scholar
Birch, S. F. & Eggers, J. M. 1972 A critical review of the experimental data for developed turbulent free shear layers. NASA SP-321 vol. 1.
Dash, S. M. & Thorpe, R. D. 1978 A new shock-capturing/shock fitting computational model for analyzing supersonic inviscid flow. ARAP Rep. No. 366.
Dash, S. M. & Wolf, D. E. 1983 Shock-capturing parabolized Navier-Stokes model for the analysis of turbulent underexpanded jets. AIAA paper 83-704.
Eggers, J. M. 1966 Velocity profile and eddy viscosity distributions downstream of a Mach 2.2 nozzle exhausting to quiescent air. NASA TN D-3601.
Harper-Bourne, M. & Fisher, M. J. 1973 The noise from shock waves in supersonic jets. AGARD Conf. Proc. 131.
Lau, J. C. 1981 Effects of exit Mach number and temperature on mean flow and turbulence characteristics in round jets. J. Fluid Mech. 105, 193218.Google Scholar
Lau, J. C., Morris, P. J. & Fisher, M. J. 1979 Measurements in subsonic and supersonic free jets using a laser velocimeter. J. Fluid Mech. 93, 127.Google Scholar
Love, E. S. 1959 Experimental and theoretical studies of axisymmetric free jets. NASA TR-R6.
Nayfeh, A. H. 1973 Perturbation Methods. Wiley-Interscience.
Norum, T. D. & Seiner, J. M. 1982a Broadband shock noise from supersonic jets. AIAA J. 20, 6873.Google Scholar
Norum, T. D. & Seiner, J. M. 1982b Measurements of mean static pressure and far field acoustics of shock-containing supersonic jets. NASA TM 84521.
Pack, D. C. 1950 A note on Prandtl's formula for the wavelength of a supersonic gas jet. Q. J. Mech. Appl. Maths 3, 173181.Google Scholar
Prandtl, L. 1904 Über die stationären Wellen in einem Gasstrahl. Phys. Zeit. 5, 599601.Google Scholar
Salas, M. D. 1974 The numerical calculation of inviscid plume flow fields. AIAA paper no. 74-523.
Schlichting, H. 1960 Boundary layer theory. McGraw-Hill.
Seiner, J. M., Dash, S. M. & Wolf, D. E. 1983 Shock noise features using the SCIPVIS code. AIAA paper no. 83-0705.
Seiner, J. M. & Norum, T. D. 1979 Experiments of shock associated noise on supersonic jets. AIAA paper no. 79-1526.
Seiner, J. M. & Norum, T. D. 1980 Aerodynamic aspects of shock containing jet plumes. AIAA paper no. 80-0965.
Seiner, J. M. & Yu, J. E. 1981 Acoustic near field and local flow properties associated with broadband shock noise. AIAA paper no. 81-1975.
Tam, C. K. W. 1972 On the noise of a nearly ideally expanded supersonic jet. J. Fluid Mech. 51, 6995.Google Scholar
Tam, C. K. W. 1975 Supersonic jet noise generated by large scale disturbances. J. Sound Vib. 38, 5179.Google Scholar
Tam, C. K. W. & Tanna, H. K. 1982 Shock associated noise of supersonic jets from convergent-divergent nozzles. J. Sound Vib. 81, 337358.Google Scholar