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    Seasonal Mesoscale and Submesoscale Eddy Variability along the North Pacific Subtropical Countercurrent

    Source: Journal of Physical Oceanography:;2014:;Volume( 044 ):;issue: 012::page 3079
    Author:
    Qiu, Bo
    ,
    Chen, Shuiming
    ,
    Klein, Patrice
    ,
    Sasaki, Hideharu
    ,
    Sasai, Yoshikazu
    DOI: 10.1175/JPO-D-14-0071.1
    Publisher: American Meteorological Society
    Abstract: ocated at the center of the western North Pacific Subtropical Gyre, the Subtropical Countercurrent (STCC) is not only abundant in mesoscale eddies, but also exhibits prominent submesoscale eddy features. Output from a ° high-resolution OGCM simulation and a gridded satellite altimetry product are analyzed to contrast the seasonal STCC variability in the mesoscale versus submesoscale ranges. Resolving the eddy scales of >150 km, the altimetry product reveals that the STCC eddy kinetic energy and rms vorticity have a seasonal maximum in May and April, respectively, a weak positive vorticity skewness without seasonal dependence, and an inverse (forward) kinetic energy cascade for wavelengths larger (shorter) than 250 km. In contrast, the submesoscale-resolving OGCM simulation detects that the STCC eddy kinetic energy and rms vorticity both appear in March, a large positive vorticity skewness with strong seasonality, and an intense inverse kinetic energy cascade whose short-wave cutoff migrates seasonally between the 35- and 100-km wavelengths. Using a 2.5-layer, reduced-gravity model with an embedded surface density gradient, the authors show that these differences are due to the seasonal evolution of two concurring baroclinic instabilities. Extracting its energy from the surface density gradient, the frontal instability has a growth time scale of O(7) days, a dominant wavelength of O(50) km, and is responsible for the surface-intensified submesoscale eddy signals. The interior baroclinic instability, on the other hand, extracts energy from the vertically sheared STCC system. It has a slow growth time scale of O(40) days, a dominant wavelength of O(250) km, and, together with the kinetic energy cascaded upscale from the submesoscales, determines the mesoscale eddy modulations.
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      Seasonal Mesoscale and Submesoscale Eddy Variability along the North Pacific Subtropical Countercurrent

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    contributor authorQiu, Bo
    contributor authorChen, Shuiming
    contributor authorKlein, Patrice
    contributor authorSasaki, Hideharu
    contributor authorSasai, Yoshikazu
    date accessioned2017-06-09T17:20:48Z
    date available2017-06-09T17:20:48Z
    date copyright2014/12/01
    date issued2014
    identifier issn0022-3670
    identifier otherams-83573.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4226813
    description abstractocated at the center of the western North Pacific Subtropical Gyre, the Subtropical Countercurrent (STCC) is not only abundant in mesoscale eddies, but also exhibits prominent submesoscale eddy features. Output from a ° high-resolution OGCM simulation and a gridded satellite altimetry product are analyzed to contrast the seasonal STCC variability in the mesoscale versus submesoscale ranges. Resolving the eddy scales of >150 km, the altimetry product reveals that the STCC eddy kinetic energy and rms vorticity have a seasonal maximum in May and April, respectively, a weak positive vorticity skewness without seasonal dependence, and an inverse (forward) kinetic energy cascade for wavelengths larger (shorter) than 250 km. In contrast, the submesoscale-resolving OGCM simulation detects that the STCC eddy kinetic energy and rms vorticity both appear in March, a large positive vorticity skewness with strong seasonality, and an intense inverse kinetic energy cascade whose short-wave cutoff migrates seasonally between the 35- and 100-km wavelengths. Using a 2.5-layer, reduced-gravity model with an embedded surface density gradient, the authors show that these differences are due to the seasonal evolution of two concurring baroclinic instabilities. Extracting its energy from the surface density gradient, the frontal instability has a growth time scale of O(7) days, a dominant wavelength of O(50) km, and is responsible for the surface-intensified submesoscale eddy signals. The interior baroclinic instability, on the other hand, extracts energy from the vertically sheared STCC system. It has a slow growth time scale of O(40) days, a dominant wavelength of O(250) km, and, together with the kinetic energy cascaded upscale from the submesoscales, determines the mesoscale eddy modulations.
    publisherAmerican Meteorological Society
    titleSeasonal Mesoscale and Submesoscale Eddy Variability along the North Pacific Subtropical Countercurrent
    typeJournal Paper
    journal volume44
    journal issue12
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/JPO-D-14-0071.1
    journal fristpage3079
    journal lastpage3098
    treeJournal of Physical Oceanography:;2014:;Volume( 044 ):;issue: 012
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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