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    Maintenance of Quasi-Stationary Waves in a Two-Level Quasi-Geostrophic Spectral Model with Topography

    Source: Journal of the Atmospheric Sciences:;1980:;Volume( 037 ):;issue: 001::page 29
    Author:
    Yao, Mao-Sung
    DOI: 10.1175/1520-0469(1980)037<0029:MOQSWI>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The maintenance of the quasi-stationary waves obtained through numerically integrating a two-level quasi-geostrophic spectral model on a ?-plane is studied. An idealized topography which has only wave-number n in the zonal direction and the first mode in the meridional direction is used to force the quasi-stationary waves. However, the model's motion contains wavenumbers 0, n and 2n in the zonal direction, while the first three modes in the meridional direction are allowed for each wave. The cases n = 2 and n = 3 are considered. The mechanism for maintaining the quasi-stationary waves is investigated by varying the imposed thermal equilibrium temperature gradient, ?Te, and the reciprocal of the internal frictional coefficient, 0.5 kI?1. If the flow is not highly irregular, the available potential energy of quasi-stationary waves (As) is maintained by the energy conversion Az?AS, where Az is the available potential energy of the time-averaged zonal mean flow. For n = 3 and moderately large ?Te and kI?1, the kinetic energy of these waves (Ks) is maintained by the energy conversion As?Ks. If ?Te, or kI?1 is smaller while n=3, kinetic energy is supplied to the quasi-stationary waves by the energy conversion Kz?Ks through the topographic forcing, where Kz is the kinetic energy of the time-averaged zonal mean flow. The latter mechanism also maintains the kinetic energy of the quasi-stationary waves for n=2 with relatively small ?Te and kI?1 is sufficiently large, the flow is highly irregular and a unique regime cannot be defined for either n = 2 or n = 3. In the case of n = 3 and moderately large ?Te and kI?1, the energy cycle, spectra and form of the quasi-stationary waves suggest that the quasi-stationary waves are largely baroclinic waves which draw their energy from the forced waves.
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      Maintenance of Quasi-Stationary Waves in a Two-Level Quasi-Geostrophic Spectral Model with Topography

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4153760
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    contributor authorYao, Mao-Sung
    date accessioned2017-06-09T14:21:10Z
    date available2017-06-09T14:21:10Z
    date copyright1980/01/01
    date issued1980
    identifier issn0022-4928
    identifier otherams-17823.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4153760
    description abstractThe maintenance of the quasi-stationary waves obtained through numerically integrating a two-level quasi-geostrophic spectral model on a ?-plane is studied. An idealized topography which has only wave-number n in the zonal direction and the first mode in the meridional direction is used to force the quasi-stationary waves. However, the model's motion contains wavenumbers 0, n and 2n in the zonal direction, while the first three modes in the meridional direction are allowed for each wave. The cases n = 2 and n = 3 are considered. The mechanism for maintaining the quasi-stationary waves is investigated by varying the imposed thermal equilibrium temperature gradient, ?Te, and the reciprocal of the internal frictional coefficient, 0.5 kI?1. If the flow is not highly irregular, the available potential energy of quasi-stationary waves (As) is maintained by the energy conversion Az?AS, where Az is the available potential energy of the time-averaged zonal mean flow. For n = 3 and moderately large ?Te and kI?1, the kinetic energy of these waves (Ks) is maintained by the energy conversion As?Ks. If ?Te, or kI?1 is smaller while n=3, kinetic energy is supplied to the quasi-stationary waves by the energy conversion Kz?Ks through the topographic forcing, where Kz is the kinetic energy of the time-averaged zonal mean flow. The latter mechanism also maintains the kinetic energy of the quasi-stationary waves for n=2 with relatively small ?Te and kI?1 is sufficiently large, the flow is highly irregular and a unique regime cannot be defined for either n = 2 or n = 3. In the case of n = 3 and moderately large ?Te and kI?1, the energy cycle, spectra and form of the quasi-stationary waves suggest that the quasi-stationary waves are largely baroclinic waves which draw their energy from the forced waves.
    publisherAmerican Meteorological Society
    titleMaintenance of Quasi-Stationary Waves in a Two-Level Quasi-Geostrophic Spectral Model with Topography
    typeJournal Paper
    journal volume37
    journal issue1
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1980)037<0029:MOQSWI>2.0.CO;2
    journal fristpage29
    journal lastpage43
    treeJournal of the Atmospheric Sciences:;1980:;Volume( 037 ):;issue: 001
    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