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    A Severe Frontal Rainband. Part III: Derived Thermodynamic Structure

    Source: Journal of the Atmospheric Sciences:;1987:;Volume( 044 ):;issue: 012::page 1615
    Author:
    Parsons, David B.
    ,
    Mohr, Carl G.
    ,
    Gal-Chen, Tzvi
    DOI: 10.1175/1520-0469(1987)044<1615:ASFRPI>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Pressure, buoyancy and virtual potential temperature perturbations are calculated from wind fields derived from Doppler radar data taken in a surface cold front. The dynamics of the front are similar to a density current This hypothesis is also suggested by accompanying numerical simulations of cold air outflows. The updraft at the leading edge of the cold air mass is maintained in conjunction with an upward directed pressure force. The average maximum updraft is in excess of 7 m s?1 without any appreciable potential instability present in the ?undisturbed? warm-sector sounding. The buoyancy and virtual potential temperature data reveal a front with a substantial fraction of the cooling taking place within the first 2 km of a frontal zone. Thus, the aspect ratio (width/depth) of the front, even after the filtering associated with the interpolation and retrieval process, is slightly less than one. The frontogenesis for the shear in the along-front wind and the thermal gradient are discussed. The gradient of these quantities in the lower levels is maintained by confluence and eventually destroyed by tilting of the gradients into the horizontal. The thermal fields are locally influenced by diabatic processes in the frontal updraft and behind the front. The cooling taking place in the cold air is apparently related to evaporation and melting of hydrormeteors. The virtual potential temperature reduction with this cooling is in excess of 0.5 K. Considerable along-front variations in the pressure, wind, and precipitation field occur due to the presence of a 13-km wave. These variations in the wind field are due to the influence of the waves of the rate of frontogenesis experienced by a parcel as it moves through the frontal zone. The primary factor for the changes in frontogenesis in the direction parallel to the surface front is the variation in the confluence term.
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      A Severe Frontal Rainband. Part III: Derived Thermodynamic Structure

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/4155684
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    • Journal of the Atmospheric Sciences

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    contributor authorParsons, David B.
    contributor authorMohr, Carl G.
    contributor authorGal-Chen, Tzvi
    date accessioned2017-06-09T14:27:24Z
    date available2017-06-09T14:27:24Z
    date copyright1987/06/01
    date issued1987
    identifier issn0022-4928
    identifier otherams-19555.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4155684
    description abstractPressure, buoyancy and virtual potential temperature perturbations are calculated from wind fields derived from Doppler radar data taken in a surface cold front. The dynamics of the front are similar to a density current This hypothesis is also suggested by accompanying numerical simulations of cold air outflows. The updraft at the leading edge of the cold air mass is maintained in conjunction with an upward directed pressure force. The average maximum updraft is in excess of 7 m s?1 without any appreciable potential instability present in the ?undisturbed? warm-sector sounding. The buoyancy and virtual potential temperature data reveal a front with a substantial fraction of the cooling taking place within the first 2 km of a frontal zone. Thus, the aspect ratio (width/depth) of the front, even after the filtering associated with the interpolation and retrieval process, is slightly less than one. The frontogenesis for the shear in the along-front wind and the thermal gradient are discussed. The gradient of these quantities in the lower levels is maintained by confluence and eventually destroyed by tilting of the gradients into the horizontal. The thermal fields are locally influenced by diabatic processes in the frontal updraft and behind the front. The cooling taking place in the cold air is apparently related to evaporation and melting of hydrormeteors. The virtual potential temperature reduction with this cooling is in excess of 0.5 K. Considerable along-front variations in the pressure, wind, and precipitation field occur due to the presence of a 13-km wave. These variations in the wind field are due to the influence of the waves of the rate of frontogenesis experienced by a parcel as it moves through the frontal zone. The primary factor for the changes in frontogenesis in the direction parallel to the surface front is the variation in the confluence term.
    publisherAmerican Meteorological Society
    titleA Severe Frontal Rainband. Part III: Derived Thermodynamic Structure
    typeJournal Paper
    journal volume44
    journal issue12
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1987)044<1615:ASFRPI>2.0.CO;2
    journal fristpage1615
    journal lastpage1631
    treeJournal of the Atmospheric Sciences:;1987:;Volume( 044 ):;issue: 012
    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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