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Journal ArticleDOI

Radiation damping of inertial oscillations in the upper ocean

T. H. Bell
- 27 Sep 1978 - 
- Vol. 88, Iss: 02, pp 289-308
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TLDR
In this paper, an energy flux of 1-10 erg/cm2 s was estimated for a relatively short (wavelength of order 2πU0/N) high frequency (of order, but less than, N) internal waves.
Abstract
Turbulent motions within the wind-mixed layer, which is advected by near-surface inertial oscillations, excite internal gravity waves in the underlying ocean layers. Momentum transport in the radiated wave field results in a drag force on the inertial currents. Because the magnitude of the inertial currents is large compared with the turbulence intensity, the resultant rate of dissipation of inertial oscillation energy is approximately equal to the energy flux in the radiated wave field. Using linear internal wave theory, asymptotic results are derived for the energy flux in terms of the Brunt-Vaisala frequency N below the mixed layer, the magnitude U0 of the inertial current, the integral length scale l of the mixed-layer turbulence and the mean-square displacement 〈ζ20〉 of the base of the mixed layer. For representative conditions, we estimate an energy flux of 1-10 erg/cm2 s into relatively short (wavelength of order 2πU0/N) high frequency (of order, but less than, N) internal waves. The resultant decay times for inertial oscillation energy range from a day to a week or so, in agreement with reported observations on the decay of inertial oscillations in the upper ocean. The estimated energy flux is comparable in magnitude to estimates for other internal wave generation mechanisms, indicating that, in addition to being a significant sink of inertial energy, this process may locally represent a significant source of internal wave energy in the open ocean.

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Citations
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Internal waves in the ocean

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Toward regional characterizations of the oceanic internal wavefield

TL;DR: In this article, the authors present numerical solutions of the resonant kinetic equation, however, that are inconsistent with the Garrett and Munk model representing a stationary state, either alone or in combination with other physical mechanisms.
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Models of the oceanic internal wave field

TL;DR: In this paper, a review of the wave field in terms of vertically progressive waves (WKB waves) as well as standing modes is presented, and it is shown that the interrelation between forcing and dissipation is controlled by internal transfer by wave-wave interactions which are very efficient in relaxing spectral distortions to the observed universal form.
References
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Journal ArticleDOI

Space-Time scales of internal waves

TL;DR: In this paper, a model E(α, ω) α μ−1ω−p+1(ω 2−ω i 2)−++ for the distribution of internal wave energy in horizontal wavenumber, frequency-space, with wavenumbers α extending to some upper limit μ(ω) α ω r-1 (ω 2 −ω i 1 2)½, and frequency ω extending from the inertial frequency i to the local Vaisala frequency n(y).
Journal ArticleDOI

The deepening of the wind-Mixed layer

TL;DR: In this article, a simple model is given that describes the response of the upper ocean to an imposed wind stress, which is taken to mix thoroughly a layer of depth h, and to erode the stably stratified fluid below.
Journal ArticleDOI

Comparison between observed and simulated wind-generated inertial oscillations

TL;DR: In this article, a simple model of forcing by a wind stress was used to estimate the phase, amplitude and intermittency of bursts of inertial oscillations in the mixed layer.
Journal ArticleDOI

Topographically generated internal waves in the open ocean

TL;DR: In this paper, the authors considered the generation of internal waves by the interaction of deep ocean flows with bottom topography and found that the internal wave drag and associated momentum flux of roughly ½ dyn/cm2, which is comparable to the average wind stress on the ocean surface.
Journal ArticleDOI

Lee waves in stratified flows with simple harmonic time dependence

TL;DR: In this article, the process of internal gravity wave generation by the simple harmonic flow (U = U0, cos ω0t) of a stably stratified fluid over an obstacle is investigated in some detail.
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