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    A Probability Box Model of a Convective Ocean

    Source: Journal of Physical Oceanography:;1997:;Volume( 027 ):;issue: 012::page 2576
    Author:
    Ikeda, M.
    DOI: 10.1175/1520-0485(1997)027<2576:APBMOA>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: A new modeling approach is proposed for representing a subpolar ocean, whose upper layer is partly convected with the lower layer. A simple box model, built as a reference, has one active box to be the upper layer of a colder ocean, which interacts with the warmer box and the lower box. The active box receives atmospheric forcing (cooling and precipitation) and a parameterized freshwater (or sea ice) flux as well, while the other boxes have their properties fixed. The active box, interacting with the warmer box, possesses a thermal-driven state, at which the warmer water enters the active box, is cooled by the atmosphere, and becomes denser. The lower box adds another solution: a convected state appears in the vicinity of the nonconvected state. The nonconvected state either separates from or is absorbed into the convected state; that is, the entire upper box is convected with the lower box, once the lower-box density is close to the upper-box density. The new component to the simple model is a probability distribution function (PDF) on the temperature?salinity (T?S) plane for the active box. The PDF in this probability box model represents heterogeneity in the upper layer, whereas one box has to be homogeneous in an ordinary box model. A T?S distribution retains only the probabilities of different water types, while their locations are discarded. The mechanisms to increase and reduce heterogeneity are modeled by the divergence and convergence of the PDF on the T?S plane, respectively. The heterogeneity is generated by the intrusion of exterior water as well as variability in the atmospheric forcing and freshwater flux, while the heterogeneity is reduced by horizontal diffusion within the box. Convection with the lower box tends to concentrate the PDF to the T, S of the lower box. Under the exterior condition that could produce both nonconvected and convected states in the simple box model, there is only one state of the upper box, which is partly convected, in the probability model. This intermediate state is possible when the divergent mechanism is intense, and the convergent mechanism is weak. Thus, the on?off convection in the simple box model is replaced with an intermediate state between the convected and the nonconvected states. It is suggested that, once mesoscale variability maintains heterogeneity, convection in the subpolar ocean is more robust against freshwater input.
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      A Probability Box Model of a Convective Ocean

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    contributor authorIkeda, M.
    date accessioned2017-06-09T14:52:48Z
    date available2017-06-09T14:52:48Z
    date copyright1997/12/01
    date issued1997
    identifier issn0022-3670
    identifier otherams-28806.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4165963
    description abstractA new modeling approach is proposed for representing a subpolar ocean, whose upper layer is partly convected with the lower layer. A simple box model, built as a reference, has one active box to be the upper layer of a colder ocean, which interacts with the warmer box and the lower box. The active box receives atmospheric forcing (cooling and precipitation) and a parameterized freshwater (or sea ice) flux as well, while the other boxes have their properties fixed. The active box, interacting with the warmer box, possesses a thermal-driven state, at which the warmer water enters the active box, is cooled by the atmosphere, and becomes denser. The lower box adds another solution: a convected state appears in the vicinity of the nonconvected state. The nonconvected state either separates from or is absorbed into the convected state; that is, the entire upper box is convected with the lower box, once the lower-box density is close to the upper-box density. The new component to the simple model is a probability distribution function (PDF) on the temperature?salinity (T?S) plane for the active box. The PDF in this probability box model represents heterogeneity in the upper layer, whereas one box has to be homogeneous in an ordinary box model. A T?S distribution retains only the probabilities of different water types, while their locations are discarded. The mechanisms to increase and reduce heterogeneity are modeled by the divergence and convergence of the PDF on the T?S plane, respectively. The heterogeneity is generated by the intrusion of exterior water as well as variability in the atmospheric forcing and freshwater flux, while the heterogeneity is reduced by horizontal diffusion within the box. Convection with the lower box tends to concentrate the PDF to the T, S of the lower box. Under the exterior condition that could produce both nonconvected and convected states in the simple box model, there is only one state of the upper box, which is partly convected, in the probability model. This intermediate state is possible when the divergent mechanism is intense, and the convergent mechanism is weak. Thus, the on?off convection in the simple box model is replaced with an intermediate state between the convected and the nonconvected states. It is suggested that, once mesoscale variability maintains heterogeneity, convection in the subpolar ocean is more robust against freshwater input.
    publisherAmerican Meteorological Society
    titleA Probability Box Model of a Convective Ocean
    typeJournal Paper
    journal volume27
    journal issue12
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/1520-0485(1997)027<2576:APBMOA>2.0.CO;2
    journal fristpage2576
    journal lastpage2588
    treeJournal of Physical Oceanography:;1997:;Volume( 027 ):;issue: 012
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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