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    On the Influence of Bottom Topography on the Agulhas Eddy

    Source: Journal of Physical Oceanography:;1996:;Volume( 026 ):;issue: 006::page 892
    Author:
    Kamenkovich, Vladimir M.
    ,
    Leonov, Yurii P.
    ,
    Nechaev, Dmitrii A.
    ,
    Byrne, Deirdre A.
    ,
    Gordon, Arnold L.
    DOI: 10.1175/1520-0485(1996)026<0892:OTIOBT>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: A series of numerical experiments with a two-layer primitive equation model is presented to study the dynamics of Agulhas eddies. The main goal of the paper is to examine the influence of an underwater meridional ridge (modeled after the Walvis Ridge) on an Agulhas eddy hitting it. First, the propagation of an eddy of the specified vertical structure over a flat bottom is considered, varying the initial eddy horizontal scale from 40 to 120 km. Unlike small nonlinear eddies, large nonlinear eddies (on the scale of Agulhas eddies) do not rapidly evolve into a compensated state (no motion in the lower layer). Second, the influence of a ridge on eddies of differing vertical structures having a specified intensity in the upper layer and a prescribed horizontal scale is analyzed. Significantly baroclinic eddies can cross the Walvis Ridge, but barotropic or near-barotropic ones cannot. The evolution of eddies crossing the ridge is compared with that of initially identical eddies moving over a flat bottom and with field observations. Eddies in our model tend toward the compensated state, with a motionless lower layer, when they cross a steep ridge. This tendency appears largely independent of the initial state of the eddy. Eddies crossing the ridge, show an intensification just before the eddy center encounters the ridge, expressed as a deepening of the thermocline depth and a heightening of the sea surface elevation. This effect is large enough [O(10 cm)] that it should be noticeable in altimeter records such as the one from the Topex-Poseidon satellite. The translational speed and direction of model eddies agree with observations, even in the absence of externally prescribed large-scale currents or friction; model eddies averaged 4.6 km day?1 and moved westward. The modeled eddies proved an effective transport for passive tracers; tracers initially located near the center of the eddy were transported with practically no losses. The influence of the ridge leads to the substantial increase of the transported tracers. Model eddies show a realistic e-folding scale for amplitude decay of 2680 km. This long scale, combined with the tracer transport, indicates that Agulhas eddies, which cross the Walvis Ridge, are capable of carrying their observed thermal and salinity anomalies far into the South Atlantic subtropical gyre.
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      On the Influence of Bottom Topography on the Agulhas Eddy

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4165648
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    contributor authorKamenkovich, Vladimir M.
    contributor authorLeonov, Yurii P.
    contributor authorNechaev, Dmitrii A.
    contributor authorByrne, Deirdre A.
    contributor authorGordon, Arnold L.
    date accessioned2017-06-09T14:52:04Z
    date available2017-06-09T14:52:04Z
    date copyright1996/06/01
    date issued1996
    identifier issn0022-3670
    identifier otherams-28522.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4165648
    description abstractA series of numerical experiments with a two-layer primitive equation model is presented to study the dynamics of Agulhas eddies. The main goal of the paper is to examine the influence of an underwater meridional ridge (modeled after the Walvis Ridge) on an Agulhas eddy hitting it. First, the propagation of an eddy of the specified vertical structure over a flat bottom is considered, varying the initial eddy horizontal scale from 40 to 120 km. Unlike small nonlinear eddies, large nonlinear eddies (on the scale of Agulhas eddies) do not rapidly evolve into a compensated state (no motion in the lower layer). Second, the influence of a ridge on eddies of differing vertical structures having a specified intensity in the upper layer and a prescribed horizontal scale is analyzed. Significantly baroclinic eddies can cross the Walvis Ridge, but barotropic or near-barotropic ones cannot. The evolution of eddies crossing the ridge is compared with that of initially identical eddies moving over a flat bottom and with field observations. Eddies in our model tend toward the compensated state, with a motionless lower layer, when they cross a steep ridge. This tendency appears largely independent of the initial state of the eddy. Eddies crossing the ridge, show an intensification just before the eddy center encounters the ridge, expressed as a deepening of the thermocline depth and a heightening of the sea surface elevation. This effect is large enough [O(10 cm)] that it should be noticeable in altimeter records such as the one from the Topex-Poseidon satellite. The translational speed and direction of model eddies agree with observations, even in the absence of externally prescribed large-scale currents or friction; model eddies averaged 4.6 km day?1 and moved westward. The modeled eddies proved an effective transport for passive tracers; tracers initially located near the center of the eddy were transported with practically no losses. The influence of the ridge leads to the substantial increase of the transported tracers. Model eddies show a realistic e-folding scale for amplitude decay of 2680 km. This long scale, combined with the tracer transport, indicates that Agulhas eddies, which cross the Walvis Ridge, are capable of carrying their observed thermal and salinity anomalies far into the South Atlantic subtropical gyre.
    publisherAmerican Meteorological Society
    titleOn the Influence of Bottom Topography on the Agulhas Eddy
    typeJournal Paper
    journal volume26
    journal issue6
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/1520-0485(1996)026<0892:OTIOBT>2.0.CO;2
    journal fristpage892
    journal lastpage912
    treeJournal of Physical Oceanography:;1996:;Volume( 026 ):;issue: 006
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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