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    On the Nonexistence of a Slow Manifold

    Source: Journal of the Atmospheric Sciences:;1987:;Volume( 044 ):;issue: 020::page 2940
    Author:
    Lorenz, E. N.
    ,
    Krishnamurthy, V.
    DOI: 10.1175/1520-0469(1987)044<2940:OTNOAS>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: We define the slow manifold S in the state space of a primitive-equation model as a hypothetical invariant manifold on which there is no gravity-wave activity. and on which unique velocity-potential and streamfunction fields correspond to each isobaric-height field. We introduce a five-variable forced damped model, and show that for this model the point H representing the Hadley circulation and the two orbits forming the unstable manifold of H must lie in S if S exists. We then show that in traveling along one of these orbits one eventually encounters gravity waves, whereupon it follows that S does not exist. A measure G of gravity-wave activity is found to decrease very rapidly as the external forcing F decreases. An approximate formula is derived for G as a function of F. We show that a particular nine-variable forced damped model with orography also fails to possess a slow manifold, and we speculate as to the existence of slow manifolds in larger and more realistic models.
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      On the Nonexistence of a Slow Manifold

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    contributor authorLorenz, E. N.
    contributor authorKrishnamurthy, V.
    date accessioned2017-06-09T14:27:41Z
    date available2017-06-09T14:27:41Z
    date copyright1987/10/01
    date issued1987
    identifier issn0022-4928
    identifier otherams-19649.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4155788
    description abstractWe define the slow manifold S in the state space of a primitive-equation model as a hypothetical invariant manifold on which there is no gravity-wave activity. and on which unique velocity-potential and streamfunction fields correspond to each isobaric-height field. We introduce a five-variable forced damped model, and show that for this model the point H representing the Hadley circulation and the two orbits forming the unstable manifold of H must lie in S if S exists. We then show that in traveling along one of these orbits one eventually encounters gravity waves, whereupon it follows that S does not exist. A measure G of gravity-wave activity is found to decrease very rapidly as the external forcing F decreases. An approximate formula is derived for G as a function of F. We show that a particular nine-variable forced damped model with orography also fails to possess a slow manifold, and we speculate as to the existence of slow manifolds in larger and more realistic models.
    publisherAmerican Meteorological Society
    titleOn the Nonexistence of a Slow Manifold
    typeJournal Paper
    journal volume44
    journal issue20
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1987)044<2940:OTNOAS>2.0.CO;2
    journal fristpage2940
    journal lastpage2950
    treeJournal of the Atmospheric Sciences:;1987:;Volume( 044 ):;issue: 020
    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
    yabeshDSpacePersian