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A throttling mechanism sustaining a hole tone feedback system at very low Mach numbers

Published online by Cambridge University Press:  03 September 2012

K. Matsuura*
Affiliation:
Graduate School of Science and Engineering, Ehime University, 3 Bunkyo-cho, Matsuyama, Ehime, 790-8577, Japan
M. Nakano
Affiliation:
Institute of Fluid Science, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Miyagi, 980-8577, Japan
*
Email address for correspondence: matsuura.kazuo.mm@ehime-u.ac.jp

Abstract

This study investigates the sound produced when a jet, issued from a circular nozzle or hole in a plate, goes through a similar hole in a second plate. The sound, known as a hole tone, is encountered in many practical engineering situations. Direct computations of a hole tone feedback system were conducted. The mean velocity of the air jet was 10 m s−1. The nozzle and the end plate hole both had a diameter of 51 mm, and the impingement length between the nozzle and the end plate was 50 mm. The computational results agreed well with past experimental data in terms of qualitative vortical structures, the relationship between the most dominant hole tone peak frequency and the jet speed, and downstream growth of the mean jet profiles. Based on the computational results, the shear-layer impingement on the hole edge, the resulting propagation of pressure waves and the associated vortical structures are discussed. To extract dominant unsteady behaviours of the hole tone phenomena, a snapshot proper orthogonal decomposition (POD) analysis of pressure fluctuation fields was conducted. It was found that the pressure fluctuation fields and the time variation of mass flows through the end plate hole were dominantly expressed by the first and second POD modes, respectively. Integrating the computational results, an axisymmetric throttling mechanism linking mass flow rates through the hole, vortex impingement and global pressure propagation, is proposed.

Type
Papers
Copyright
Copyright © Cambridge University Press 2012

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References

1. Blake, W. K. 1986 Mechanics of Flow-Induced Sound and Vibration, vol. 1. Academic.Google Scholar
2. Chanaud, R. C. & Powell, A. 1965 Some experiments concerning the hole and ring tone. J. Acoust. Soc. Am. 37 (5), 902911.CrossRefGoogle Scholar
3. Chorin, A. & Marsden, J. 1992 A Mathematical Introduction to Fluid Mechanics. Springer.Google Scholar
4. Crighton, D. G. 1992 The jet edge-tone feedback cycle: linear theory for the operating stages. J. Fluid Mech. 234, 361391.CrossRefGoogle Scholar
5. Freund, J. B. 1997 Proposed inflow/outflow boundary condition for direct computation of aerodynamic sound. AIAA J. 35 (4), 740742.CrossRefGoogle Scholar
6. Gaitonde, D. V. & Visbal, M. R. 2000 Padé-type higher-order boundary filters for the Navier–Stokes equations. AIAA J. 38 (11), 21032112.CrossRefGoogle Scholar
7. Ginevsky, A. S., Vlasov, Y. V. & Karavosov, R. K. 2010 Acoustic Control of Turbulent Jets. Springer.Google Scholar
8. Holger, D. K. 1977 Fluid mechanics of the edgetone. J. Acoust. Soc. Am. 62 (5), 11161128.CrossRefGoogle Scholar
9. Howe, M. S. 1975 Contributions to the theory of aerodynamic sound, with application to excess jet noise and the theory of the flute. J. Fluid Mech. 71, 625673.CrossRefGoogle Scholar
10. Howe, M. S. 1980 The dissipation of sound at an edge. J. Sound Vib. 70 (3), 407411.CrossRefGoogle Scholar
11. Howe, M. S. 1997a Acoustics of Fluid–Structure Interactions. Cambridge University Press.Google Scholar
12. Howe, M. S. 1997b Edge, cavity and aperture tones at very low Mach numbers. J. Fluid Mech. 330, 6184.CrossRefGoogle Scholar
13. Imai, I. 1973 Fluid Dynamics, vol. 1. Syokabo.Google Scholar
14. Langthjem, M. A. & Nakano, M. 2005 A numerical simulation of the hole-tone feedback cycle based on an axisymmetric discrete vortex method and Curle’s equation. J. Sound Vib. 288 (1–2), 133176.CrossRefGoogle Scholar
15. Lele, S. K. 1992 Compact finite difference schemes with spectral-like resolution. J. Comput. Phys. 103 (1), 1642.CrossRefGoogle Scholar
16. Matsuura, K. & Kato, C. 2007 Large-eddy simulation of compressible transitional flows in a low-pressure turbine cascade. AIAA J. 45 (2), 442457.CrossRefGoogle Scholar
17. Matsuura, K. & Nakano, M. 2011 Direct computation of a hole-tone feedback system at very low Mach numbers. J. Fluid Sci. Technol. 6 (4), 548561.CrossRefGoogle Scholar
18. Michalke, A. 1984 Survey on jet instability theory. Prog. Aerosp. 21, 159199.CrossRefGoogle Scholar
19. Press, W. H., Teukolsky, S. A., Vetterling, W. T. & Flannery, B. P. 1992 Numerical Recipes in Fortran 77, second edition. Cambridge University Press.Google Scholar
20. Rai, M. M. & Moin, P. 1993 Direct numerical simulation of transition and turbulence in a spatially evolving boundary layer. J. Comput. Phys. 109 (2), 169192.CrossRefGoogle Scholar
21. Rayleigh, Lord. 1945 Theory of Sound, vol. 2. Dover.Google Scholar
22. Rockwell, D. & Naudascher, E. 1979 Self-sustained oscillations of impinging free shear layers. Annu. Rev. Fluid Mech. 11, 6794.CrossRefGoogle Scholar
23. Rossiter, J. E. 1962 The effect of cavities on the buffeting of aircraft. Royal Aircraft Establishment Technical Memorandum 754.Google Scholar
24. Sirovich, L. & Rodriguez, J. D. 1987 Coherent structures and chaos: a model problem. Phys. Lett. A 120 (5), 211214.CrossRefGoogle Scholar
25. Sondhauss, C. 1854 Ueber die beim Ausströmen der Luft enstehenden Töne. Ann. Phys. 167 (1), 126147.CrossRefGoogle Scholar
26. Student 1908 The probable error of a mean. Biometrika 6 (1), 1–25.CrossRefGoogle Scholar
27. Umeda, Y. & Ishii, R. 1986 Frequency characteristics of discrete tones generated in a high subsonic jet. AIAA J. 693695.CrossRefGoogle Scholar