| contributor author | A. V. Mirzamoghadam | |
| contributor author | Principal Engineer | |
| date accessioned | 2017-05-09T00:02:23Z | |
| date available | 2017-05-09T00:02:23Z | |
| date copyright | April, 2000 | |
| date issued | 2000 | |
| identifier issn | 1528-8919 | |
| identifier other | JETPEZ-26795#364_1.pdf | |
| identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/123674 | |
| description 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? | |
| publisher | The American Society of Mechanical Engineers (ASME) | |
| title | 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 | |
| type | Journal Paper | |
| journal volume | 122 | |
| journal issue | 2 | |
| journal title | Journal of Engineering for Gas Turbines and Power | |
| identifier doi | 10.1115/1.483218 | |
| journal fristpage | 364 | |
| identifier eissn | 0742-4795 | |
| keywords | Heat transfer | |
| keywords | Bearings | |
| keywords | Gas turbines AND Geometry | |
| tree | Journal of Engineering for Gas Turbines and Power:;2000:;volume( 122 ):;issue: 002 | |
| contenttype | Fulltext | |