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Acoustic forcing of oblique wave resonance in the far wake

Published online by Cambridge University Press:  26 April 2006

C. H. K. Williamson
Affiliation:
Mechanical and Aerospace Engineering, Upson Hall, Cornell University, Ithaca, NY 14853, USA
A. Prasad
Affiliation:
Mechanical and Aerospace Engineering, Upson Hall, Cornell University, Ithaca, NY 14853, USA

Abstract

In this paper, we investigate to what extent the far-wake ‘signature’ of the near-wake vortex dynamics of a nominally two-dimensional bluff body is affected by the character of the free-stream noise. We confirm the existence of an oblique wave resonance (at frequency, fKfT), which is caused by nonlinear ‘quadratic’ interactions between primary oblique shedding waves (fK) and secondary two-dimensional waves (fT), which are amplified from free-stream disturbances. In this work, oblique wave resonance is induced by acoustic forcing of two-dimensional waves. The use of acoustic forcing reveals a set of higher-order oblique wave resonances corresponding to frequencies (fKnfT), where n is an integer. We find from visualization that, even when the secondary two-dimensional waves have the same frequency as the oblique waves, it is the oblique waves that are preferentially amplified. Oblique wave angles up to 74° have been observed. The response of the wake to a large range of forcing frequencies shows a broad region of peak response, centred around F = (fT/fK) = 0.55, and is in reasonable agreement with predictions from linear stability analysis. A similar broad response is found for each of the higher-order oblique wave modes. Simple equations for the oblique waves yield approximate conditions for maximum wake response, with a frequency for peak response given by Fmax = 1/2n = 1/2, 1/4, 1/6,…, and an oblique wave angle given by θmax = 2θK, where θK is the angle of oblique vortex shedding. An increase in forcing amplitude has the effect of bringing the nonlinear wave interactions, leading to oblique wave resonance, further upstream. Paradoxically, the effect of an increase in amplitude (A) of the two-dimensional wave forcing is to further amplify the oblique waves in preference to the two-dimensional waves and, under some conditions, to inhibit the appearance of prominent two-dimensional waves where they would otherwise appear. With a variation in forcing amplitude, the amplitude of oblique wave response is found to be closely proportional to A½. In summary, this investigation confirms the surprising result that it is only through the existence of noise in the free stream that the far wake is ‘connected’ to the near wake.

Type
Research Article
Copyright
© 1993 Cambridge University Press

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References

Cimbala, J. M. 1984 Large structure in the far wakes of two-dimensional bluff bodies. PhD thesis, Graduate Aeronautical Laboratories, California Institute of Technology.
Cimbala, J. M. & Krein, A. 1990 Effect of freestream conditions on the far wake of a cylinder. AIAA J. 28, 1369.Google Scholar
Cimbala, J. M., Nagib, H. M. & Roshko, A. 1988 Large structure in the far wakes of two-dimensional bluff bodies. J. Fluid Mech. 190, 265.Google Scholar
Corke, T., Krull, J. D. & Ghassemi, M. 1992 Three-dimensional mode resonance in far wakes. J. Fluid Mech. 239, 99.Google Scholar
Desruelle, D. 1983 Beyond the Karman vortex street. MS thesis, Illinois Institute of Technology, Chicago.
Eisenlohr, H. & Eckelmann, H. 1989 Vortex splitting and its consequences in the vortex street wake of cylinders at low Reynolds number. Phys. Fluids A 1, 189.Google Scholar
Flemming, M. F. 1987 Secondary instability in the far wake. MS thesis, Illinois Institute of Technology, Chicago.
Hammache, M. & Gharib, M. 1989 A novel method to promote parallel shedding in the wake of circular cylinders. Phys. Fluids A 1, 1611.Google Scholar
Hammache, M. & Gharib, M. 1991 An experimental study of the parallel and oblique vortex shedding from circular cylinders. J. Fluid Mech. 232, 567.Google Scholar
Hammache, M. & Gharib, M. 1992 On the evolution of three-dimensionalities in laminar bluff body wakes. In Proc. IUTAM Conf. on Bluff Body Wake Instabilities (ed. H. Eckelmann & J. M. R. Graham). Springer (to appear.)
Koenig, M., Eisenlohr, H., Eckelmann, H. 1990 The fine structure in the S-Re relationship of the laminar wake of a circular cylinder. Phys. Fluids A 2, 1607.Google Scholar
Lasheras, J. C. & Meiburg, E. 1990 Three-dimensional vorticity modes in the wake of a flat plate. Phys. Fluids A 2, 371.Google Scholar
Matsui, T. & Okude, M. 1981 Vortex pairing in a Karman vortex street. In Proc. Seventh Biennial Symp. on Turbulence, Rolla, Missouri.
Matsui, T. & Okude, M. 1983 Formation of the secondarty vortex street in the wake of a circular cylinder. In Structure of Complex Turbulent Shear Flow, IUTAM Symp., Marseille, 1982. Springer.
Meiburg, E. 1987 On the role of subharmonic perturbations in the far wake. J. Fluid Mech. 177, 83.Google Scholar
Meiburg, E. 1992 The three-dimensional evolution of oblique waves in plane wakes. In Proc. IUTAM Conf. on Bluff Body Wake Instabilities (ed. H. Eckelmann & J. M. R. Graham). Springer (to appear.)
Squire, H. B. 1933 On the stability for three-dimensional disturbances of viscous fluid flow between parallel walls. Proc. R. Soc. Lond A 142, 621.Google Scholar
Taneda, S. 1959 Downstream development of wakes behind cylinders. J. Phys. Soc. Japan 14, 843.Google Scholar
Williamson, C. H. K. 1988 Defining a universal and continuous Strouhal–Reynolds number relationship for the laminar vortex shedding of a circular cylinder. Phys. Fluids 31, 2742.Google Scholar
Williamson, C. H. K. 1989 Oblique and parallel modes of vortex shedding in the wake of a circular cylinder at low Reynolds numbers. J. Fluid Mech. 206, 579.Google Scholar
Williamson, C. H. K. 1992 Wave interactions in the far wake. In Proc. IUTAM Conf. on Bluff Body Wake Instabilities (ed. H. Eckelmann & J. M. R. Graham). Springer (to appear.)
Williamson, C. H. K. & Prasad, A. 1993a A new mechanism for oblique wave resonance in the ‘natural’ far wake. J. Fluid Mech. 256, 269 (referred to herein as WP.)Google Scholar
Williamson, C. H. K. & Prasad, A. 1993b Oblique wave interactions in the far wake. Phys Fluids A 5, 1854.Google Scholar