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    Non-Stationary Finite-Amplitude Convection in a Thin Fluid Layer Bounded by a Stably Stratified Region

    Source: Journal of the Atmospheric Sciences:;1971:;Volume( 028 ):;issue: 008::page 1389
    Author:
    Ogura, Yoshimitsu
    ,
    Yagihashi, Akiko
    DOI: 10.1175/1520-0469(1971)028<1389:NSFACI>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Numerical integrations are performed for the equations governing two-dimensional convection flows in a fluid confined between two horizontal plates. A situation considered here is that local heating at a time-independent rate is provided at the middle level of the fluid so that the upper half of the fluid is destabilized and the lower half stabilized. It is shown that steady-state solutions are obtained when the Rayleigh number (R) is 1.1 times Rc (critical Rayleigh number at which convection sets in according to the linearized theory). For three cases where R=1.5 Rc, 2 Rc and 3 Rc, time-dependent solutions are obtained which describe extremely regular and repeatable convection flows. The flow pattern is such that plume-like cells generated by heating move horizontally, merge with neighboring plumes, and new plumes are generated. This process is repeated. Time-dependent but irregular solutions are obtained for R=5 Rc and beyond.
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      Non-Stationary Finite-Amplitude Convection in a Thin Fluid Layer Bounded by a Stably Stratified Region

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4151813
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    • Journal of the Atmospheric Sciences

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    contributor authorOgura, Yoshimitsu
    contributor authorYagihashi, Akiko
    date accessioned2017-06-09T14:16:09Z
    date available2017-06-09T14:16:09Z
    date copyright1971/11/01
    date issued1971
    identifier issn0022-4928
    identifier otherams-16070.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4151813
    description abstractNumerical integrations are performed for the equations governing two-dimensional convection flows in a fluid confined between two horizontal plates. A situation considered here is that local heating at a time-independent rate is provided at the middle level of the fluid so that the upper half of the fluid is destabilized and the lower half stabilized. It is shown that steady-state solutions are obtained when the Rayleigh number (R) is 1.1 times Rc (critical Rayleigh number at which convection sets in according to the linearized theory). For three cases where R=1.5 Rc, 2 Rc and 3 Rc, time-dependent solutions are obtained which describe extremely regular and repeatable convection flows. The flow pattern is such that plume-like cells generated by heating move horizontally, merge with neighboring plumes, and new plumes are generated. This process is repeated. Time-dependent but irregular solutions are obtained for R=5 Rc and beyond.
    publisherAmerican Meteorological Society
    titleNon-Stationary Finite-Amplitude Convection in a Thin Fluid Layer Bounded by a Stably Stratified Region
    typeJournal Paper
    journal volume28
    journal issue8
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1971)028<1389:NSFACI>2.0.CO;2
    journal fristpage1389
    journal lastpage1399
    treeJournal of the Atmospheric Sciences:;1971:;Volume( 028 ):;issue: 008
    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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