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contributor authorSmyth, W. D.
contributor authorNash, J. D.
contributor authorMoum, J. N.
date accessioned2017-06-09T17:17:47Z
date available2017-06-09T17:17:47Z
date copyright2005/06/01
date issued2005
identifier issn0022-3670
identifier otherams-82617.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4225751
description abstractDirect numerical simulations are used to compare turbulent diffusivities of heat and salt during the growth and collapse of Kelvin?Helmholtz billows. The ratio of diffusivities is obtained as a function of buoyancy Reynolds number Reb and of the density ratio R? (the ratio of the contributions of heat and salt to the density stratification). The diffusivity ratio is generally less than unity (heat is mixed more effectively than salt), but it approaches unity with increasing Reb and also with increasing R?. Instantaneous diffusivity ratios near unity are achieved during the most turbulent phase of the event even when Reb is small; much of the Reb dependence results from the fact that, at higher Reb, the diffusivity ratio remains close to unity for a longer time after the turbulence decays. An explanation for this is proposed in terms of the Batchelor scaling for scalar fields. Results are interpreted in terms of the dynamics of turbulent Kelvin?Helmholtz billows, and are compared in detail with previous studies of differential diffusion in numerical, laboratory, and observational contexts. The overall picture suggests that the diffusivities become approximately equal when Reb exceeds O(102). The effect of R? is significant only when Reb is less than this value.
publisherAmerican Meteorological Society
titleDifferential Diffusion in Breaking Kelvin–Helmholtz Billows
typeJournal Paper
journal volume35
journal issue6
journal titleJournal of Physical Oceanography
identifier doi10.1175/JPO2739.1
journal fristpage1004
journal lastpage1022
treeJournal of Physical Oceanography:;2005:;Volume( 035 ):;issue: 006
contenttypeFulltext


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