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    Density Variation and Isopycnic Layers

    Source: Journal of Applied Meteorology:;1964:;volume( 003 ):;issue: 003::page 290
    Author:
    Smith, J. W.
    DOI: 10.1175/1520-0450(1964)003<0290:DVAIL>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: A pole-to-pole study of density deviations near the 80th meridian west is presented from the surface to 31 km altitude. Density deviations are greatest at the surface, and under extreme conditions may range from 1.0 to 2.0 kg m?2. Density decreases almost exponentially with altitude and occasionally falls below 0.01 kg m?3 at 31 km. Density deviations decrease from the surface to an isopycnic layer, which varies in height from 6 km in polar regions to 12 km at the equator. Above this isopycnic layer, density variations increase with altitude to a maximum density deviation layer. This maximum density deviation layer occurs along the base of the summer tropopause and is approximately the center of the tropospheric wind maximum. The maximum density deviation layer is parallel to, and 50 per cent higher in altitude than the lower isopycnic layer. A weaker, second isopycnic layer is shown above and parallel to the maximum density deviation layer; this second isopycnic layer is found in tropical regions and near the south pole. Because of large seasonal and latitudinal variations in atmospheric density, no single standard atmosphere can present density data adequate for high speed vehicle operations on a global basis.
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      Density Variation and Isopycnic Layers

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    contributor authorSmith, J. W.
    date accessioned2017-06-09T16:36:27Z
    date available2017-06-09T16:36:27Z
    date copyright1964/06/01
    date issued1964
    identifier issn0021-8952
    identifier otherams-7083.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4212656
    description abstractA pole-to-pole study of density deviations near the 80th meridian west is presented from the surface to 31 km altitude. Density deviations are greatest at the surface, and under extreme conditions may range from 1.0 to 2.0 kg m?2. Density decreases almost exponentially with altitude and occasionally falls below 0.01 kg m?3 at 31 km. Density deviations decrease from the surface to an isopycnic layer, which varies in height from 6 km in polar regions to 12 km at the equator. Above this isopycnic layer, density variations increase with altitude to a maximum density deviation layer. This maximum density deviation layer occurs along the base of the summer tropopause and is approximately the center of the tropospheric wind maximum. The maximum density deviation layer is parallel to, and 50 per cent higher in altitude than the lower isopycnic layer. A weaker, second isopycnic layer is shown above and parallel to the maximum density deviation layer; this second isopycnic layer is found in tropical regions and near the south pole. Because of large seasonal and latitudinal variations in atmospheric density, no single standard atmosphere can present density data adequate for high speed vehicle operations on a global basis.
    publisherAmerican Meteorological Society
    titleDensity Variation and Isopycnic Layers
    typeJournal Paper
    journal volume3
    journal issue3
    journal titleJournal of Applied Meteorology
    identifier doi10.1175/1520-0450(1964)003<0290:DVAIL>2.0.CO;2
    journal fristpage290
    journal lastpage298
    treeJournal of Applied Meteorology:;1964:;volume( 003 ):;issue: 003
    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