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    Entropy Generation In the Ocean by Small-Scale Mixing

    Source: Journal of Physical Oceanography:;1984:;Volume( 014 ):;issue: 004::page 688
    Author:
    Gregg, M. C.
    DOI: 10.1175/1520-0485(1984)014<0688:EGITOB>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: An expression that includes salt diffusion was developed and evaluated for the rate of entropy production σ in the ocean. The evaluation was done for mixing events produced by turbulent overturns and double diffusion. Temperature and salinity profiles from four representative oceanic regimes were used in the evaluation. For typical mid- or low-latitude profiles thermal diffusion is the main component of σ in upper-ocean turbulent events; in abyssal waters, viscous dissipation is the principal component. The depth of transition from dominance by σt to dominance by σv depends upon the depth dependence of mixing intensity, which has not been determined. Salt diffusion plays a major role only in a few locations where salinity strongly dominates the density field; the most prominent example is the shallow arctic halocline. Elsewhere, the effect of salt diffusion, However, when the viscous dissipation within the well-mixed layers above and below salt-fingering interfaces is also considered, viscous dissipation may be the dominant factor. The possible effect of viscous dissipation and the heat of mixing in the heat equation is also considered and found to be negligible unless strong turbulent dissipation rates are found in the bottom boundary layer, or intense mixing events occur in arctic haloclines.
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      Entropy Generation In the Ocean by Small-Scale Mixing

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    contributor authorGregg, M. C.
    date accessioned2017-06-09T14:47:03Z
    date available2017-06-09T14:47:03Z
    date copyright1984/04/01
    date issued1984
    identifier issn0022-3670
    identifier otherams-26684.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4163605
    description abstractAn expression that includes salt diffusion was developed and evaluated for the rate of entropy production σ in the ocean. The evaluation was done for mixing events produced by turbulent overturns and double diffusion. Temperature and salinity profiles from four representative oceanic regimes were used in the evaluation. For typical mid- or low-latitude profiles thermal diffusion is the main component of σ in upper-ocean turbulent events; in abyssal waters, viscous dissipation is the principal component. The depth of transition from dominance by σt to dominance by σv depends upon the depth dependence of mixing intensity, which has not been determined. Salt diffusion plays a major role only in a few locations where salinity strongly dominates the density field; the most prominent example is the shallow arctic halocline. Elsewhere, the effect of salt diffusion, However, when the viscous dissipation within the well-mixed layers above and below salt-fingering interfaces is also considered, viscous dissipation may be the dominant factor. The possible effect of viscous dissipation and the heat of mixing in the heat equation is also considered and found to be negligible unless strong turbulent dissipation rates are found in the bottom boundary layer, or intense mixing events occur in arctic haloclines.
    publisherAmerican Meteorological Society
    titleEntropy Generation In the Ocean by Small-Scale Mixing
    typeJournal Paper
    journal volume14
    journal issue4
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/1520-0485(1984)014<0688:EGITOB>2.0.CO;2
    journal fristpage688
    journal lastpage711
    treeJournal of Physical Oceanography:;1984:;Volume( 014 ):;issue: 004
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
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