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    The Evolution of Three-Peak Raindrop Size Distributions in One-Dimensional Shaft Models. Part II: Multiple Pulse Rain

    Source: Journal of the Atmospheric Sciences:;1991:;Volume( 048 ):;issue: 013::page 1587
    Author:
    McFarquhar, Greg M.
    ,
    List, Roland
    DOI: 10.1175/1520-0469(1991)048<1587:TEOTPR>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: The release of multiple pulses of rain with durations of 120 s < T < 600 s and pulse repetition periods of 240 s < &tau < 1200 s at the top of one-dimensional shafts, followed by drop coalescence and breakup during the fall, leads to the arrival of drops in overlapping packages at the ground, with the largest drops first in the individual packages. When the drop spectra are averaged over time, three-peak distributions (3PDs) are found. More frequent and shorter pulses produce 3PDs that resemble three-peak equilibrium distributions (3PED) for steady warm rain closer than less frequent longer pulses because overlapping pulses lead to more interactions between large and small drops. When a 3PED is released at shaft top, it disappears because different size drops fall at different speeds, and then must be recreated by drop interactions. These multiple pulses replicate trends measured during nonsteady tropical rain better than single pulses. A ?pulse interference diameter,? based on the parameterization of single pulse rain, describes how much interaction occurs between pulses.
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      The Evolution of Three-Peak Raindrop Size Distributions in One-Dimensional Shaft Models. Part II: Multiple Pulse Rain

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4156805
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    contributor authorMcFarquhar, Greg M.
    contributor authorList, Roland
    date accessioned2017-06-09T14:30:27Z
    date available2017-06-09T14:30:27Z
    date copyright1991/07/01
    date issued1991
    identifier issn0022-4928
    identifier otherams-20563.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4156805
    description abstractThe release of multiple pulses of rain with durations of 120 s < T < 600 s and pulse repetition periods of 240 s < &tau < 1200 s at the top of one-dimensional shafts, followed by drop coalescence and breakup during the fall, leads to the arrival of drops in overlapping packages at the ground, with the largest drops first in the individual packages. When the drop spectra are averaged over time, three-peak distributions (3PDs) are found. More frequent and shorter pulses produce 3PDs that resemble three-peak equilibrium distributions (3PED) for steady warm rain closer than less frequent longer pulses because overlapping pulses lead to more interactions between large and small drops. When a 3PED is released at shaft top, it disappears because different size drops fall at different speeds, and then must be recreated by drop interactions. These multiple pulses replicate trends measured during nonsteady tropical rain better than single pulses. A ?pulse interference diameter,? based on the parameterization of single pulse rain, describes how much interaction occurs between pulses.
    publisherAmerican Meteorological Society
    titleThe Evolution of Three-Peak Raindrop Size Distributions in One-Dimensional Shaft Models. Part II: Multiple Pulse Rain
    typeJournal Paper
    journal volume48
    journal issue13
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1991)048<1587:TEOTPR>2.0.CO;2
    journal fristpage1587
    journal lastpage1595
    treeJournal of the Atmospheric Sciences:;1991:;Volume( 048 ):;issue: 013
    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