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    Dynamics of Storm Tracks: A Linear Instability Perspective

    Source: Journal of the Atmospheric Sciences:;1995:;Volume( 052 ):;issue: 006::page 697
    Author:
    Lee, Woo-Jin
    ,
    Mak, Maniun
    DOI: 10.1175/1520-0469(1995)052<0697:DOSTAL>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The instability properties of an observed seasonal mean flow are diagnosed in terms of (i) the local versus global instability of normal modes, (ii) the convective versus absolute instability of a pulse, and (iii) the finite-time instability of optimal structures (modes), so as to learn about the dynamics of the storm tracks. The analysis is carried out in the context of the boreal winter circulation of 1982?83 with the use of a three-layer hemispheric linear balanced model. Four clusters of normal modes with different geographical characteristics are identified among the unstable modes with an e-folding time shorter than 8 days. The Pacific modes and Atlantic modes bear a striking resemblance to the Pacific and Atlantic storm tracks of that winter, respectively. The Pacific mode primarily arises from convective instability, but recycling feedback around the hemisphere is not essential. Self-seeding of such a mode stems from an upstream convergence of ageostrophic geopotential flux over the western Pacific and may be interpreted as a manifestation of weak absolute instability. The advection of perturbation energy by the diffluent basic flow is the major process of redistributing substantial energy to the far downstream region in such a mode. A typical Atlantic mode has a much more extensive spatial structure. It is a global mode because its existence requires the process of recycling feedback around the hemisphere. Absolute instability is also found possible in the observed basic flow. It gives rise to two other local modes, one over East Asia and the other over West Africa. There are a large number of amplifying optimal modes for an optimization time (τ) up to 10 days. The 1-day optimal mode could give rise to an intensification rate for one day exceeding that of the most unstable normal mode by sixfold. An Atlantic adjoint mode would optimally evolve to approximately an Atlantic mode in about 15 days, whereas a Pacific adjoint mode would optimally evolve to a Pacific mode in less than 10 days.
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      Dynamics of Storm Tracks: A Linear Instability Perspective

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4157737
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    contributor authorLee, Woo-Jin
    contributor authorMak, Maniun
    date accessioned2017-06-09T14:32:52Z
    date available2017-06-09T14:32:52Z
    date copyright1995/03/01
    date issued1995
    identifier issn0022-4928
    identifier otherams-21401.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4157737
    description abstractThe instability properties of an observed seasonal mean flow are diagnosed in terms of (i) the local versus global instability of normal modes, (ii) the convective versus absolute instability of a pulse, and (iii) the finite-time instability of optimal structures (modes), so as to learn about the dynamics of the storm tracks. The analysis is carried out in the context of the boreal winter circulation of 1982?83 with the use of a three-layer hemispheric linear balanced model. Four clusters of normal modes with different geographical characteristics are identified among the unstable modes with an e-folding time shorter than 8 days. The Pacific modes and Atlantic modes bear a striking resemblance to the Pacific and Atlantic storm tracks of that winter, respectively. The Pacific mode primarily arises from convective instability, but recycling feedback around the hemisphere is not essential. Self-seeding of such a mode stems from an upstream convergence of ageostrophic geopotential flux over the western Pacific and may be interpreted as a manifestation of weak absolute instability. The advection of perturbation energy by the diffluent basic flow is the major process of redistributing substantial energy to the far downstream region in such a mode. A typical Atlantic mode has a much more extensive spatial structure. It is a global mode because its existence requires the process of recycling feedback around the hemisphere. Absolute instability is also found possible in the observed basic flow. It gives rise to two other local modes, one over East Asia and the other over West Africa. There are a large number of amplifying optimal modes for an optimization time (τ) up to 10 days. The 1-day optimal mode could give rise to an intensification rate for one day exceeding that of the most unstable normal mode by sixfold. An Atlantic adjoint mode would optimally evolve to approximately an Atlantic mode in about 15 days, whereas a Pacific adjoint mode would optimally evolve to a Pacific mode in less than 10 days.
    publisherAmerican Meteorological Society
    titleDynamics of Storm Tracks: A Linear Instability Perspective
    typeJournal Paper
    journal volume52
    journal issue6
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1995)052<0697:DOSTAL>2.0.CO;2
    journal fristpage697
    journal lastpage723
    treeJournal of the Atmospheric Sciences:;1995:;Volume( 052 ):;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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