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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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