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    Propagation and Breaking at High Altitudes of Gravity Waves Excited by Tropospheric Forcing

    Source: Journal of the Atmospheric Sciences:;1996:;Volume( 053 ):;issue: 015::page 2186
    Author:
    Prusa, Joseph M.
    ,
    Smolarkiewicz, Piotr K.
    ,
    Garcia, Rolando R.
    DOI: 10.1175/1520-0469(1996)053<2186:PABAHA>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: An anelastic approximation is used with a time-variable coordinate transformation to formulate a two-dimensional numerical model that describes the evolution of gravity waves. The model is solved using a semi-Lagrangian method with monotone (nonoscillatory) interpolation of all advected fields. The time-variable transformation is used to generate disturbances at the lower boundary that approximate the effect of a traveling line of thunderstorms (a squall line) or of flow over a broad topographic obstacle. The vertical propagation and breaking of the gravity wave field (under conditions typical of summer solstice) is illustrated for each of these cases. It is shown that the wave field at high altitudes is dominated by a single horizontal wavelength, which is not always related simply to the horizontal dimension of the source. The morphology of wave breaking depends on the horizontal wavelength; for sufficiently short waves, breaking involves roughly one half of the wavelength. In common with other studies, it is found that the breaking waves undergo ?self-acceleration,? such that the Zonal-mean intrinsic frequency remains approximately constant in spite of large changes in the background wind. It is also shown that many of the features obtained in the calculations can be understood in terms of linear wave theory. In particular, linear theory provides insights into the wavelength of the waves that break at high altitudes, the onset and evolution of breaking, the horizontal extent of the breaking region and its position relative to the forcing, and the minimum and maximum altitudes where breaking occurs. Wave breaking ceases at the altitude where the background dissipation rate (which in our model is a proxy for molecular diffusion) becomes greater than the rate of dissipation due to wave breaking. This altitude, in effect, the model turbopause, is shown to depend on a relatively small number of parameters that characterize the waves and the background state.
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      Propagation and Breaking at High Altitudes of Gravity Waves Excited by Tropospheric Forcing

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4158189
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    • Journal of the Atmospheric Sciences

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    contributor authorPrusa, Joseph M.
    contributor authorSmolarkiewicz, Piotr K.
    contributor authorGarcia, Rolando R.
    date accessioned2017-06-09T14:34:00Z
    date available2017-06-09T14:34:00Z
    date copyright1996/08/01
    date issued1996
    identifier issn0022-4928
    identifier otherams-21809.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4158189
    description abstractAn anelastic approximation is used with a time-variable coordinate transformation to formulate a two-dimensional numerical model that describes the evolution of gravity waves. The model is solved using a semi-Lagrangian method with monotone (nonoscillatory) interpolation of all advected fields. The time-variable transformation is used to generate disturbances at the lower boundary that approximate the effect of a traveling line of thunderstorms (a squall line) or of flow over a broad topographic obstacle. The vertical propagation and breaking of the gravity wave field (under conditions typical of summer solstice) is illustrated for each of these cases. It is shown that the wave field at high altitudes is dominated by a single horizontal wavelength, which is not always related simply to the horizontal dimension of the source. The morphology of wave breaking depends on the horizontal wavelength; for sufficiently short waves, breaking involves roughly one half of the wavelength. In common with other studies, it is found that the breaking waves undergo ?self-acceleration,? such that the Zonal-mean intrinsic frequency remains approximately constant in spite of large changes in the background wind. It is also shown that many of the features obtained in the calculations can be understood in terms of linear wave theory. In particular, linear theory provides insights into the wavelength of the waves that break at high altitudes, the onset and evolution of breaking, the horizontal extent of the breaking region and its position relative to the forcing, and the minimum and maximum altitudes where breaking occurs. Wave breaking ceases at the altitude where the background dissipation rate (which in our model is a proxy for molecular diffusion) becomes greater than the rate of dissipation due to wave breaking. This altitude, in effect, the model turbopause, is shown to depend on a relatively small number of parameters that characterize the waves and the background state.
    publisherAmerican Meteorological Society
    titlePropagation and Breaking at High Altitudes of Gravity Waves Excited by Tropospheric Forcing
    typeJournal Paper
    journal volume53
    journal issue15
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1996)053<2186:PABAHA>2.0.CO;2
    journal fristpage2186
    journal lastpage2216
    treeJournal of the Atmospheric Sciences:;1996:;Volume( 053 ):;issue: 015
    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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