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    Isolated Waves and Eddies in a Shallow Water Model

    Source: Journal of Physical Oceanography:;1984:;Volume( 014 ):;issue: 006::page 1047
    Author:
    Davey, Michael K.
    ,
    Killworth, Peter D.
    DOI: 10.1175/1520-0485(1984)014<1047:IWAEIA>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: A shallow-water beta-channel model was used to carry out numerical experiments with cyclonic and anticyclonic disturbances of various strengths. The model is inviscid, so fluid elements conserve potential vorticity q when unforced. Regions of closed q contours correspond to Lagrangian (material) eddies. (All fluid within a Lagrangian eddy travels with the eddy?in contrast to regions of closed height contours.) Motion is wavelike for very weak disturbances (maximum particle speed ?; ? long planetary wave speed ?). The height field disperses like a group of linear Rossby waves, and tracers have small, oscillatory (mainly north-south) displacements, with very little scatter. When ?≈?, the planetary q field is sufficiently distorted for small Lagrangian eddies to appear. Very small eddies are simply bodily advected by the linear wave field. Small eddies are to some extent ?self propelling?: they move westward and north (cyclone) or south (anticyclone), moving fluid elements towards their ?rest? latitudes. Tracers within such eddies are moved away from neighboring tracers initially outside the eddy (which have largely wavelike motion). The eddy and the height extremum, initially together, gradually separate. (The position of a height extremum is not a good indicator of tracer movement.) When Ü??, the q field is grossly distorted, and the motion is dominated by a nonlinear eddy which is strong enough to advect ambient q (and fluid elements) around itself. This wrapping effect leads to relatively strong mixing (by wave breaking?) around the fringes of the eddy, which slowly decays by this mechanism. Movement of the eddy is predominantly westward, at almost the same speed as the center-of-mass anomaly (for a buoyancy-generated disturbance). Analytic center-of-mass calculations predict that the center-of-mass of an anticyclone travels westward faster than the linear long-wave speed ?, whereas a cyclone travels slower than ?. The predictions are confirmed by the numerical experiments. Some estimates of mixing based on tracer separation are given.
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      Isolated Waves and Eddies in a Shallow Water Model

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    contributor authorDavey, Michael K.
    contributor authorKillworth, Peter D.
    date accessioned2017-06-09T14:47:07Z
    date available2017-06-09T14:47:07Z
    date copyright1984/06/01
    date issued1984
    identifier issn0022-3670
    identifier otherams-26712.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4163637
    description abstractA shallow-water beta-channel model was used to carry out numerical experiments with cyclonic and anticyclonic disturbances of various strengths. The model is inviscid, so fluid elements conserve potential vorticity q when unforced. Regions of closed q contours correspond to Lagrangian (material) eddies. (All fluid within a Lagrangian eddy travels with the eddy?in contrast to regions of closed height contours.) Motion is wavelike for very weak disturbances (maximum particle speed ?; ? long planetary wave speed ?). The height field disperses like a group of linear Rossby waves, and tracers have small, oscillatory (mainly north-south) displacements, with very little scatter. When ?≈?, the planetary q field is sufficiently distorted for small Lagrangian eddies to appear. Very small eddies are simply bodily advected by the linear wave field. Small eddies are to some extent ?self propelling?: they move westward and north (cyclone) or south (anticyclone), moving fluid elements towards their ?rest? latitudes. Tracers within such eddies are moved away from neighboring tracers initially outside the eddy (which have largely wavelike motion). The eddy and the height extremum, initially together, gradually separate. (The position of a height extremum is not a good indicator of tracer movement.) When Ü??, the q field is grossly distorted, and the motion is dominated by a nonlinear eddy which is strong enough to advect ambient q (and fluid elements) around itself. This wrapping effect leads to relatively strong mixing (by wave breaking?) around the fringes of the eddy, which slowly decays by this mechanism. Movement of the eddy is predominantly westward, at almost the same speed as the center-of-mass anomaly (for a buoyancy-generated disturbance). Analytic center-of-mass calculations predict that the center-of-mass of an anticyclone travels westward faster than the linear long-wave speed ?, whereas a cyclone travels slower than ?. The predictions are confirmed by the numerical experiments. Some estimates of mixing based on tracer separation are given.
    publisherAmerican Meteorological Society
    titleIsolated Waves and Eddies in a Shallow Water Model
    typeJournal Paper
    journal volume14
    journal issue6
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/1520-0485(1984)014<1047:IWAEIA>2.0.CO;2
    journal fristpage1047
    journal lastpage1064
    treeJournal of Physical Oceanography:;1984:;Volume( 014 ):;issue: 006
    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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