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contributor authorArdhuin, Fabrice
contributor authorJenkins, Alastair D.
date accessioned2017-06-09T17:18:05Z
date available2017-06-09T17:18:05Z
date copyright2006/03/01
date issued2006
identifier issn0022-3670
identifier otherams-82740.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4225887
description abstractThe phase-averaged energy evolution for random surface waves interacting with oceanic turbulence is investigated. The change in wave energy balances the change in the production of turbulent kinetic energy (TKE). Outside the surface viscous layer and the bottom boundary layer the turbulent flux is not related to the wave-induced shear so that eddy viscosity parameterizations cannot be applied. Instead, it is assumed that the wave motion and the turbulent fluxes are not correlated on the scale of the wave period. Using a generalized Lagrangian average it is found that the mean wave-induced shears, despite zero vorticity, yield a production of TKE as if the Stokes drift shear were a mean flow shear. This result provides a new interpretation of a previous derivation from phase-averaged equations by McWilliams et al. It is found that the present source or sink of wave energy is smaller but is still on the order of the empirically adjusted functions used for the dissipation of swell energy in operational wave models, as well as observations of that phenomenon by Snodgrass et al.
publisherAmerican Meteorological Society
titleOn the Interaction of Surface Waves and Upper Ocean Turbulence
typeJournal Paper
journal volume36
journal issue3
journal titleJournal of Physical Oceanography
identifier doi10.1175/JPO2862.1
journal fristpage551
journal lastpage557
treeJournal of Physical Oceanography:;2006:;Volume( 036 ):;issue: 003
contenttypeFulltext


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