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Turbulent structure beneath surface gravity waves sheared by the wind

Published online by Cambridge University Press:  26 April 2006

L. Thais  and
J. Magnaudet
L. Thais
Affiliation:
Institut de Mécanique des Fluides de Toulouse, UMR CNRS 5502, 2 Avenue Camille Soula, 31400 Toulouse, France Present address: School of Mathematics, University of Bristol, Bristol, BS8 1TW, UK.
J. Magnaudet
Affiliation:
Institut de Mécanique des Fluides de Toulouse, UMR CNRS 5502, 2 Avenue Camille Soula, 31400 Toulouse, France
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Abstract

New experiments have been carried out in a large laboratory channel to explore the structure of turbulent motion in the water layer beneath surface gravity waves. These experiments involve pure wind waves as well as wind-ruffled mechanically generated waves. A submersible two-component LDV system has been used to obtain the three components of the instantaneous velocity field along the vertical direction at a single fetch of 26 m. The displacement of the free surface has been determined simultaneously at the same downstream location by means of wave gauges. For both types of waves, suitable separation techniques have been used to split the total fluctuating motion into an orbital contribution (i.e. a motion induced by the displacement of the surface) and a turbulent contribution. Based on these experimental results, the present paper focuses on the structure of the water turbulence. The most prominent feature revealed by the two sets of experiments is the enhancement of both the turbulent kinetic energy and its dissipation rate with respect to values found near solid walls. Spectral analysis provides clear indications that wave–turbulence interactions greatly affect energy transfers over a significant frequency range by imposing a constant timescale related to the wave-induced strain. For mechanical waves we discuss several turbulent statistics and their modulation with respect to the wave phase, showing that the turbulence we observed was deeply affected at both large and small scales by the wave motion. An analysis of the phase variability of the bursting suggests that there is a direct interaction between the waves and the underlying turbulence, mainly at the wave crests. Turbulence budgets show that production essentially takes place in the wavy region of the flow, i.e. above the wave troughs. These results are finally used to address the nature of the basic mechanisms governing wave–turbulence interactions.

Type
Research Article
Information
Journal of Fluid Mechanics , Volume 328 , 10 December 1996 , pp. 313 - 344
Copyright
© 1996 Cambridge University Press

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