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    Mechanism of Heating and the Boundary Layer over the Tibetan Plateau

    Source: Monthly Weather Review:;1994:;volume( 122 ):;issue: 002::page 305
    Author:
    Yanai, Michio
    ,
    Li, Chengfeng
    DOI: 10.1175/1520-0493(1994)122<0305:MOHATB>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The structure of the boundary layer and the mechanism of heating over the Tibetan Plateau are examined using the data obtained from the First GARP (Global Atmospheric Research Program) Global Experiment and the Chinese Qinghai?Xizang (Tibet) Plateau Meteorological Experiment from May to August 1979. The meteorological elements near the plateau surface exhibit pronounced diurnal variations. There is a large ground?air temperature difference during the daytime generating a thin layer of superadiabatic lapse rates near the surface. The horizontal wind speed attains the minimum in the morning and the maximum in the evening. A deep and well-mixed layer of potential temperature is observed over the western and central plateau in the evening (1200 UTC). However, moisture is not well mixed vertically and water vapor mixing ratio is larger in the morning (0000 UTC) than in the evening. The mixed layer becomes shallower from the western to the central plateau and it disappears over the eastern plateau. There is a deep layer of large-scale ascent over the plateau. The upward motion and convective activity over the plateau are more intense in the evening than in the morning. Before the onset of summer rains, sensible heat flux from the surface is the major source of heating on the plateau. The analysis of the ground?air temperature difference supports the hypothesis that dry convective elements rising from the heated surface provide the mechanism for tropospheric heating during this period. After the onset of the summer rains, however, the heat released by condensation is the primary source of heating over the eastern plateau. During the dry preonset period, the diabatic heating in the boundary layer is nearly balanced with the cold horizontal advection due to the prevailing westerly wind above the plateau. After the onset, the adiabatic cooling due to strong upward motions nearly balances with the heat released by condensation. The dry horizontal advection plays an important role in the moisture balance of the boundary layer.
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      Mechanism of Heating and the Boundary Layer over the Tibetan Plateau

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/4203219
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    • Monthly Weather Review

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    contributor authorYanai, Michio
    contributor authorLi, Chengfeng
    date accessioned2017-06-09T16:09:47Z
    date available2017-06-09T16:09:47Z
    date copyright1994/02/01
    date issued1994
    identifier issn0027-0644
    identifier otherams-62338.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4203219
    description abstractThe structure of the boundary layer and the mechanism of heating over the Tibetan Plateau are examined using the data obtained from the First GARP (Global Atmospheric Research Program) Global Experiment and the Chinese Qinghai?Xizang (Tibet) Plateau Meteorological Experiment from May to August 1979. The meteorological elements near the plateau surface exhibit pronounced diurnal variations. There is a large ground?air temperature difference during the daytime generating a thin layer of superadiabatic lapse rates near the surface. The horizontal wind speed attains the minimum in the morning and the maximum in the evening. A deep and well-mixed layer of potential temperature is observed over the western and central plateau in the evening (1200 UTC). However, moisture is not well mixed vertically and water vapor mixing ratio is larger in the morning (0000 UTC) than in the evening. The mixed layer becomes shallower from the western to the central plateau and it disappears over the eastern plateau. There is a deep layer of large-scale ascent over the plateau. The upward motion and convective activity over the plateau are more intense in the evening than in the morning. Before the onset of summer rains, sensible heat flux from the surface is the major source of heating on the plateau. The analysis of the ground?air temperature difference supports the hypothesis that dry convective elements rising from the heated surface provide the mechanism for tropospheric heating during this period. After the onset of the summer rains, however, the heat released by condensation is the primary source of heating over the eastern plateau. During the dry preonset period, the diabatic heating in the boundary layer is nearly balanced with the cold horizontal advection due to the prevailing westerly wind above the plateau. After the onset, the adiabatic cooling due to strong upward motions nearly balances with the heat released by condensation. The dry horizontal advection plays an important role in the moisture balance of the boundary layer.
    publisherAmerican Meteorological Society
    titleMechanism of Heating and the Boundary Layer over the Tibetan Plateau
    typeJournal Paper
    journal volume122
    journal issue2
    journal titleMonthly Weather Review
    identifier doi10.1175/1520-0493(1994)122<0305:MOHATB>2.0.CO;2
    journal fristpage305
    journal lastpage323
    treeMonthly Weather Review:;1994:;volume( 122 ):;issue: 002
    contenttypeFulltext
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