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    Discussion: “Internal Bearing Chamber Wall Heat Transfer as a Function of Operating Conditions and Chamber Geometry” [ASME J. Eng. Gas Turbines Power, 122, No. 2, pp. 314–320]1

    Source: Journal of Engineering for Gas Turbines and Power:;2000:;volume( 122 ):;issue: 002::page 364
    Author:
    A. V. Mirzamoghadam
    ,
    Principal Engineer
    DOI: 10.1115/1.483218
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The subject under investigation is very important to the gas turbine industry, and the derivation of a correlation for the oil chamber wall heat transfer coefficient is long past overdue. The complexity, however, is that the correlation needs to represent the two-phase flow regime (liquid oil + air) along the chamber wall which changes with engine operating conditions. Therefore, the proposed correlation in this paper requires further validation in order to delineate the effect of two-phase flow regime. Would the authors comment on why the definition of the Reynolds number (Eq. (12)) is not based on local tangential velocity (ns×rs) but rather a pseudo tangential velocity based on circumference (ns×2πrs). Also, if the chamber circumference is U=πDh, why are the Reynolds numbers of Eqs. (15) and (16) written without the π?
    keyword(s): Heat transfer , Bearings , Gas turbines AND Geometry ,
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      Discussion: “Internal Bearing Chamber Wall Heat Transfer as a Function of Operating Conditions and Chamber Geometry” [ASME J. Eng. Gas Turbines Power, 122, No. 2, pp. 314–320]1

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    http://yetl.yabesh.ir/yetl1/handle/yetl/123674
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    contributor authorA. V. Mirzamoghadam
    contributor authorPrincipal Engineer
    date accessioned2017-05-09T00:02:23Z
    date available2017-05-09T00:02:23Z
    date copyrightApril, 2000
    date issued2000
    identifier issn1528-8919
    identifier otherJETPEZ-26795#364_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/123674
    description abstractThe subject under investigation is very important to the gas turbine industry, and the derivation of a correlation for the oil chamber wall heat transfer coefficient is long past overdue. The complexity, however, is that the correlation needs to represent the two-phase flow regime (liquid oil + air) along the chamber wall which changes with engine operating conditions. Therefore, the proposed correlation in this paper requires further validation in order to delineate the effect of two-phase flow regime. Would the authors comment on why the definition of the Reynolds number (Eq. (12)) is not based on local tangential velocity (ns×rs) but rather a pseudo tangential velocity based on circumference (ns×2πrs). Also, if the chamber circumference is U=πDh, why are the Reynolds numbers of Eqs. (15) and (16) written without the π?
    publisherThe American Society of Mechanical Engineers (ASME)
    titleDiscussion: “Internal Bearing Chamber Wall Heat Transfer as a Function of Operating Conditions and Chamber Geometry” [ASME J. Eng. Gas Turbines Power, 122, No. 2, pp. 314–320]1
    typeJournal Paper
    journal volume122
    journal issue2
    journal titleJournal of Engineering for Gas Turbines and Power
    identifier doi10.1115/1.483218
    journal fristpage364
    identifier eissn0742-4795
    keywordsHeat transfer
    keywordsBearings
    keywordsGas turbines AND Geometry
    treeJournal of Engineering for Gas Turbines and Power:;2000:;volume( 122 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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