The influence of surface gravity waves on the injection of turbulence in the upper ocean
Observations were made in the near-surface layer, at about 8 m depth in 132 m deep water off the coast of Ålesund in Norway, for a duration of 2.5 months in late 2011. The measurement period covers the passage of two low pressure systems with substantial wind and wave forcing. The time series of the...
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2014-06-01
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Series: | Nonlinear Processes in Geophysics |
Online Access: | http://www.nonlin-processes-geophys.net/21/713/2014/npg-21-713-2014.pdf |
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doaj-cde44e3dbd054e2ebd2854805fe91d552020-11-24T23:46:20ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462014-06-0121371373310.5194/npg-21-713-2014The influence of surface gravity waves on the injection of turbulence in the upper oceanM. Bakhoday Paskyabi0I. Fer1Geophysical Institute, University of Bergen, Allégaten 70, 5007 Bergen, NorwayGeophysical Institute, University of Bergen, Allégaten 70, 5007 Bergen, NorwayObservations were made in the near-surface layer, at about 8 m depth in 132 m deep water off the coast of Ålesund in Norway, for a duration of 2.5 months in late 2011. The measurement period covers the passage of two low pressure systems with substantial wind and wave forcing. The time series of the dissipation rate of turbulent kinetic energy, ε, and the estimates of surface gravity waves are analysed. Dissipation rates varied by 5 orders of magnitude and reached 10<sup>-5</sup>–10<sup>-4</sup> W kg<sup>−1</sup> in conditions when wind speed exceeded 15 m s<sup>−1</sup> and the significant wave height was of the order of 10 m. The data set suggests substantial injection of turbulence from breaking surface gravity waves and Langmuir turbulence. To support and interpret the observations, numerical calculations are conducted using a second-order turbulence closure scheme based on the Mellor–Yamada level 2.5 scheme, modified to incorporate the near-surface processes such as Langmuir circulation and wave breaking. The results from a run forced by observed wind and wave fields compare favourably with the observations. Comparisons with other near-surface data sets available from the literature lend confidence on our dissipation measurements and the wave-forced simulations.http://www.nonlin-processes-geophys.net/21/713/2014/npg-21-713-2014.pdf |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. Bakhoday Paskyabi I. Fer |
spellingShingle |
M. Bakhoday Paskyabi I. Fer The influence of surface gravity waves on the injection of turbulence in the upper ocean Nonlinear Processes in Geophysics |
author_facet |
M. Bakhoday Paskyabi I. Fer |
author_sort |
M. Bakhoday Paskyabi |
title |
The influence of surface gravity waves on the injection of turbulence in the upper ocean |
title_short |
The influence of surface gravity waves on the injection of turbulence in the upper ocean |
title_full |
The influence of surface gravity waves on the injection of turbulence in the upper ocean |
title_fullStr |
The influence of surface gravity waves on the injection of turbulence in the upper ocean |
title_full_unstemmed |
The influence of surface gravity waves on the injection of turbulence in the upper ocean |
title_sort |
influence of surface gravity waves on the injection of turbulence in the upper ocean |
publisher |
Copernicus Publications |
series |
Nonlinear Processes in Geophysics |
issn |
1023-5809 1607-7946 |
publishDate |
2014-06-01 |
description |
Observations were made in the
near-surface layer, at about 8 m depth in 132 m deep water off the coast of
Ålesund in Norway, for a duration of 2.5 months in late 2011. The
measurement period covers the passage of two low pressure systems with
substantial wind and wave forcing. The time series of the dissipation rate of
turbulent kinetic energy, ε, and the estimates of surface gravity
waves are analysed. Dissipation rates varied by 5 orders of magnitude and
reached 10<sup>-5</sup>–10<sup>-4</sup> W kg<sup>−1</sup> in conditions when wind speed
exceeded 15 m s<sup>−1</sup> and the significant wave height was of the order of
10 m. The data set suggests substantial injection of turbulence from
breaking surface gravity waves and Langmuir turbulence. To support and
interpret the observations, numerical calculations are conducted using a
second-order turbulence closure scheme based on the Mellor–Yamada level 2.5
scheme, modified to incorporate the near-surface processes such as Langmuir
circulation and wave breaking. The results from a run forced by observed wind
and wave fields compare favourably with the observations. Comparisons with
other near-surface data sets available from the literature lend confidence on
our dissipation measurements and the wave-forced simulations. |
url |
http://www.nonlin-processes-geophys.net/21/713/2014/npg-21-713-2014.pdf |
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