Full Coverage Film Cooling: Film Effectiveness and Heat Transfer Coefficients for Dense Hole Arrays at Different Hole Angles, Contraction Ratios, and Blowing RatiosSource: Journal of Heat Transfer:;2013:;volume( 135 ):;issue: 003::page 31707DOI: 10.1115/1.4007981Publisher: The American Society of Mechanical Engineers (ASME)
Abstract: Experimental results are presented for a fullcoverage film cooling arrangement which simulates a portion of a gas turbine engine, with appropriate streamwise static pressure gradient. The test surface utilizes varying blowing ratio (BR) along the length of the contraction passage which contains the cooling hole arrangement. For the different experimental conditions examined, film cooling holes are sharpedged and streamwise inclined either at 20 deg or 30 deg with respect to the liner surface. The film cooling holes in adjacent streamwise rows are staggered with respect to each other. Data are provided for turbulent film cooling, contraction ratios of 1, 3, 4, and 5, blowing ratios (at the test section entrance) of 2.0, 5.0, and 10.0, coolant Reynolds numbers Refc of 10,000–12,000, freestream temperatures from 75 آ°C to 115 آ°C, a film hole diameter of 7 mm, and density ratios from 1.15 to 1.25. Nondimensional streamwise and spanwise film cooling hole spacings, X/D and Y/D, are 6, and 5, respectively. When the streamwise hole inclination angle is 20 deg spatially averaged and lineaveraged adiabatic effectiveness values at each x/D location are about the same as the contraction ratio varies between 1, 3, and 4, with slightly higher values at each x/D location when the contraction ratio Cr is 5. For each contraction ratio, there is a slight increase in effectiveness when the blowing ratio is increased from 2.0 to 5.0 but there is no further substantial improvement when the blowing ratio is increased to 10.0. Overall, lineaveraged and spatially averagedadiabatic film effectiveness data, and spatially averaged heat transfer coefficient data are described as they are affected by contraction ratio, blowing ratio, hole angle خ±, and streamwise location x/D. For example, when خ±â€‰= 20 deg, the detrimental effects of mainstream acceleration are apparent since heat transfer coefficients for contraction ratios Cr of 3 and 5 are often higher than values for Cr = 1, especially for x/D > 100.
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contributor author | Ligrani, Phil | |
contributor author | Goodro, Matt | |
contributor author | Fox, Mike | |
contributor author | Moon, Hee | |
date accessioned | 2017-05-09T00:59:33Z | |
date available | 2017-05-09T00:59:33Z | |
date issued | 2013 | |
identifier issn | 0022-1481 | |
identifier other | ht_135_3_031707.pdf | |
identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/152038 | |
description abstract | Experimental results are presented for a fullcoverage film cooling arrangement which simulates a portion of a gas turbine engine, with appropriate streamwise static pressure gradient. The test surface utilizes varying blowing ratio (BR) along the length of the contraction passage which contains the cooling hole arrangement. For the different experimental conditions examined, film cooling holes are sharpedged and streamwise inclined either at 20 deg or 30 deg with respect to the liner surface. The film cooling holes in adjacent streamwise rows are staggered with respect to each other. Data are provided for turbulent film cooling, contraction ratios of 1, 3, 4, and 5, blowing ratios (at the test section entrance) of 2.0, 5.0, and 10.0, coolant Reynolds numbers Refc of 10,000–12,000, freestream temperatures from 75 آ°C to 115 آ°C, a film hole diameter of 7 mm, and density ratios from 1.15 to 1.25. Nondimensional streamwise and spanwise film cooling hole spacings, X/D and Y/D, are 6, and 5, respectively. When the streamwise hole inclination angle is 20 deg spatially averaged and lineaveraged adiabatic effectiveness values at each x/D location are about the same as the contraction ratio varies between 1, 3, and 4, with slightly higher values at each x/D location when the contraction ratio Cr is 5. For each contraction ratio, there is a slight increase in effectiveness when the blowing ratio is increased from 2.0 to 5.0 but there is no further substantial improvement when the blowing ratio is increased to 10.0. Overall, lineaveraged and spatially averagedadiabatic film effectiveness data, and spatially averaged heat transfer coefficient data are described as they are affected by contraction ratio, blowing ratio, hole angle خ±, and streamwise location x/D. For example, when خ±â€‰= 20 deg, the detrimental effects of mainstream acceleration are apparent since heat transfer coefficients for contraction ratios Cr of 3 and 5 are often higher than values for Cr = 1, especially for x/D > 100. | |
publisher | The American Society of Mechanical Engineers (ASME) | |
title | Full Coverage Film Cooling: Film Effectiveness and Heat Transfer Coefficients for Dense Hole Arrays at Different Hole Angles, Contraction Ratios, and Blowing Ratios | |
type | Journal Paper | |
journal volume | 135 | |
journal issue | 3 | |
journal title | Journal of Heat Transfer | |
identifier doi | 10.1115/1.4007981 | |
journal fristpage | 31707 | |
journal lastpage | 31707 | |
identifier eissn | 1528-8943 | |
tree | Journal of Heat Transfer:;2013:;volume( 135 ):;issue: 003 | |
contenttype | Fulltext |