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    A Quasi-One-Dimensional, Time-Dependent and Non-Precipitating Cumulus Cloud Model: On the Bimodal Distribution of Cumulus Cloud Height

    Source: Journal of the Atmospheric Sciences:;1983:;Volume( 040 ):;issue: 003::page 651
    Author:
    Wang, John Y. C.
    DOI: 10.1175/1520-0469(1983)040<0651:AQODTD>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: A quasi-one-dimensional, lime-dependent and non-precipitating cumulus cloud model is presented. The model has a source and three regions?a core region, an immediate environmental annular region and a far-environmental region. These regions constitute a convective cell with the bottom open to the source layer below. The source layer is replaced by a circular source located directly beneath the core region, below the cloud base and above the ground. The source emits source air of specified properties at a constant rate. If the properties are good enough and the rate of emission is high, namely, a high source strength, clouds are expected to form. Through a sensitivity test composed of more than 100 different source strengths, we have discovered that there exist two critical values for the strength of the source in producing shallow and deep cumulus clouds in a given atmosphere. If the source strength is below the lower critical value, no cloud can form. Above the upper critical value, a deep cumulus cloud is produced. In between, a shallow plume cloud is produced. These two critical values are both small and close to each other. In a given atmosphere, whether a deep or a shallow cloud develops is extremely sensitive to the variation of the source strength, when the source strength is near its critical value. An important implication of our result is that a cloud can only be shallow or deep. None can be of intermediate height, unless other factors are present, such as an inversion. Applying these results, we have offered some plausible explanations to the bimodal distribution of the final heights of the cloud tops, with respect to time as observed over mountain peaks, and with respect to space as observed over tropical oceans. Also, we have attempted to clarify the conditions for the formation of shallow and deep cumulus clouds.
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      A Quasi-One-Dimensional, Time-Dependent and Non-Precipitating Cumulus Cloud Model: On the Bimodal Distribution of Cumulus Cloud Height

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4154547
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    contributor authorWang, John Y. C.
    date accessioned2017-06-09T14:23:44Z
    date available2017-06-09T14:23:44Z
    date copyright1983/03/01
    date issued1983
    identifier issn0022-4928
    identifier otherams-18531.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4154547
    description abstractA quasi-one-dimensional, lime-dependent and non-precipitating cumulus cloud model is presented. The model has a source and three regions?a core region, an immediate environmental annular region and a far-environmental region. These regions constitute a convective cell with the bottom open to the source layer below. The source layer is replaced by a circular source located directly beneath the core region, below the cloud base and above the ground. The source emits source air of specified properties at a constant rate. If the properties are good enough and the rate of emission is high, namely, a high source strength, clouds are expected to form. Through a sensitivity test composed of more than 100 different source strengths, we have discovered that there exist two critical values for the strength of the source in producing shallow and deep cumulus clouds in a given atmosphere. If the source strength is below the lower critical value, no cloud can form. Above the upper critical value, a deep cumulus cloud is produced. In between, a shallow plume cloud is produced. These two critical values are both small and close to each other. In a given atmosphere, whether a deep or a shallow cloud develops is extremely sensitive to the variation of the source strength, when the source strength is near its critical value. An important implication of our result is that a cloud can only be shallow or deep. None can be of intermediate height, unless other factors are present, such as an inversion. Applying these results, we have offered some plausible explanations to the bimodal distribution of the final heights of the cloud tops, with respect to time as observed over mountain peaks, and with respect to space as observed over tropical oceans. Also, we have attempted to clarify the conditions for the formation of shallow and deep cumulus clouds.
    publisherAmerican Meteorological Society
    titleA Quasi-One-Dimensional, Time-Dependent and Non-Precipitating Cumulus Cloud Model: On the Bimodal Distribution of Cumulus Cloud Height
    typeJournal Paper
    journal volume40
    journal issue3
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1983)040<0651:AQODTD>2.0.CO;2
    journal fristpage651
    journal lastpage664
    treeJournal of the Atmospheric Sciences:;1983:;Volume( 040 ):;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
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