Scaling turbulent dissipation in the transition layer

dc.contributor.author Sun, Oliver M. T.
dc.contributor.author Jayne, Steven R.
dc.contributor.author Polzin, Kurt L.
dc.contributor.author Rahter, Bryan A.
dc.contributor.author St. Laurent, Louis C.
dc.date.accessioned 2014-08-06T19:24:58Z
dc.date.available 2014-08-06T19:24:58Z
dc.date.issued 2013-11
dc.description Author Posting. © American Meteorological Society, 2013. This article is posted here by permission of American Meteorological Society for personal use, not for redistribution. The definitive version was published in Journal of Physical Oceanography 43 (2013): 2475–2489, doi:10.1175/JPO-D-13-057.1. en_US
dc.description.abstract Data from three midlatitude, month-long surveys are examined for evidence of enhanced vertical mixing associated with the transition layer (TL), here defined as the strongly stratified layer that exists between the well mixed layer and the thermocline below. In each survey, microstructure estimates of turbulent dissipation were collected concurrently with fine-structure stratification and shear. Survey-wide averages are formed in a “TL coordinate” zTL, which is referenced around the depth of maximum stratification for each profile. Averaged profiles show characteristic TL structures such as peaks in stratification N2 and shear variance S2, which fall off steeply above zTL = 0 and more gradually below. Turbulent dissipation rates ɛ are 5–10 times larger than those found in the upper thermocline (TC). The gradient Richardson number Ri = N2/S2 becomes unstable (Ri < 0.25) within ~10 m of the TL upper boundary, suggesting that shear instability is active in the TL for zTL > 0. Ri is stable for zTL ≤ 0. Turbulent dissipation is found to scale exponentially with depth for zTL ≤ 0, but the decay scales are different for the TL and upper TC: ɛ scales well with either N2 or S2. Owing to the strong correlation between S2 and N2, existing TC scalings of the form ɛ ~ |S|p|N|q overpredict variations in ɛ. The scale dependence of shear variance is not found to significantly affect the scalings of ɛ versus N2 and S2 for zTL ≤ 0. However, the onset of unstable Ri at the top of the TL is sensitively dependent to the resolution of the shears. en_US
dc.description.sponsorship This work was funded by NSF Grant OCE-0968787 as part of a Climate Process Team for internal wave-driven mixing. en_US
dc.format.mimetype application/pdf
dc.identifier.citation Journal of Physical Oceanography 43 (2013): 2475–2489 en_US
dc.identifier.doi 10.1175/JPO-D-13-057.1
dc.identifier.uri https://hdl.handle.net/1912/6787
dc.language.iso en_US en_US
dc.publisher American Meteorological Society en_US
dc.relation.uri https://doi.org/10.1175/JPO-D-13-057.1
dc.subject Atm/Ocean Structure/ Phenomena en_US
dc.subject Diapycnal mixing en_US
dc.subject Mixed layer en_US
dc.subject Thermocline en_US
dc.subject Physical Meteorology and Climatology en_US
dc.subject Heat budgets/fluxes en_US
dc.subject Observational techniques and algorithms en_US
dc.subject In situ oceanic observations en_US
dc.subject Profilers, oceanic en_US
dc.title Scaling turbulent dissipation in the transition layer en_US
dc.type Article en_US
dspace.entity.type Publication
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