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    Rise Height for Negatively Buoyant Fountains and Depth of Penetration for Negatively Buoyant Jets Impinging an Interface

    Source: Journal of Fluids Engineering:;2000:;volume( 122 ):;issue: 004::page 779
    Author:
    P. D. Friedman
    ,
    J. Katz
    DOI: 10.1115/1.1311786
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: A vertical jet or fountain, whose velocity is opposite to the direction of its buoyant force, reverses direction after reaching a maximum penetration depth. This penetration depth is measured from the jet exit or, if present, the location of the undisturbed interface. This paper shows that the penetration depth is only a function of a Richardson number divided by a jet spreading factor. If no interface is present, the spreading factor is one; otherwise the spreading factor is only a function of distance between the jet exit and the interface. As long as the jet is fully turbulent, the penetration depth is independent of Reynolds and Weber numbers. These trends are applicable to a broad range of fluid systems including air jets impacting liquids as well as miscible and immiscible liquid-liquid systems with only slight density differences. [S0098-2202(00)00304-7]
    keyword(s): Density , Fluids , Turbulence , Jets , Flow (Dynamics) , Air jets AND Force ,
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      Rise Height for Negatively Buoyant Fountains and Depth of Penetration for Negatively Buoyant Jets Impinging an Interface

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    https://yetl.yabesh.ir/yetl1/handle/yetl/123831
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    contributor authorP. D. Friedman
    contributor authorJ. Katz
    date accessioned2017-05-09T00:02:37Z
    date available2017-05-09T00:02:37Z
    date copyrightDecember, 2000
    date issued2000
    identifier issn0098-2202
    identifier otherJFEGA4-27157#779_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/123831
    description abstractA vertical jet or fountain, whose velocity is opposite to the direction of its buoyant force, reverses direction after reaching a maximum penetration depth. This penetration depth is measured from the jet exit or, if present, the location of the undisturbed interface. This paper shows that the penetration depth is only a function of a Richardson number divided by a jet spreading factor. If no interface is present, the spreading factor is one; otherwise the spreading factor is only a function of distance between the jet exit and the interface. As long as the jet is fully turbulent, the penetration depth is independent of Reynolds and Weber numbers. These trends are applicable to a broad range of fluid systems including air jets impacting liquids as well as miscible and immiscible liquid-liquid systems with only slight density differences. [S0098-2202(00)00304-7]
    publisherThe American Society of Mechanical Engineers (ASME)
    titleRise Height for Negatively Buoyant Fountains and Depth of Penetration for Negatively Buoyant Jets Impinging an Interface
    typeJournal Paper
    journal volume122
    journal issue4
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.1311786
    journal fristpage779
    journal lastpage782
    identifier eissn1528-901X
    keywordsDensity
    keywordsFluids
    keywordsTurbulence
    keywordsJets
    keywordsFlow (Dynamics)
    keywordsAir jets AND Force
    treeJournal of Fluids Engineering:;2000:;volume( 122 ):;issue: 004
    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