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Local isotropy and the decay of turbulence in a stratified fluid

Published online by Cambridge University Press:  20 April 2006

A. E. Gargett
Affiliation:
Institute of Ocean Sciences, Patricia Bay, P.O. Box 6000, Sidney, B.C., VSL 4B2, Canada
T. R. Osborn
Affiliation:
U.S. Naval Postgraduate School, Monterey, CA 93940, U.S.A.
P. W. Nasmyth
Affiliation:
Institute of Ocean Sciences, Patricia Bay

Abstract

The validity of the assumption of local isotropy is investigated using measurements of three orthogonal components of the turbulent velocity fields associated with initially high-Reynolds-number geophysical turbulence. The turbulent fields, generated by various large-scale internal motions caused by tidal flows over an estuarine sill, decay under the influence of stable mean density gradients. With measurements from sensors mounted on a submersible, we examine the evolution of spectral shapes and of ratios of cross-stream to streamwise components, as well as the degree of high-wavenumber universality, for the observational range of the parameter Iks/kb = lb/ls. This ratio is a measure of separation between the Kolmogoroff wavenumber ks≡ (ε/ν3)¼ ≡ 2π/ls typical of scales by which turbulent kinetic energy has been dissipated (at rate ε), and the buoyancy wavenumber kb ≡ (N3/ε)½ ≡ 2π/lb typical of scales at which the ambient stratification parameter N ≡ (−gρz0)½ becomes important. For values of I larger than ∼ 3000, inertial subranges are observed in all spectra, and the spectral ratio ϕ2211 of cross-stream to streamwise spectral densities reaches the isotropic value of 4/3 for about a decade in wavenumber. As ks/kb decreases, inertial subranges vanish, but spectra of the cross-stream and streamwise components continue to satisfy isotropic relationships at dissipation wavenumbers. We provide a criterion for when ε may safely be estimated from a single measured component of the dissipation tensor, and also explore questions of appropriate low-wavenumber normalization for buoyancy-modified turbulence.

Type
Research Article
Copyright
© 1984 Cambridge University Press

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