Numerical Simulation of Evaporating Two-Phase Flow in a High-Aspect-Ratio Microchannel with BendsSource: Journal of Heat Transfer:;2017:;volume( 139 ):;issue: 008::page 80905Author:Lee, Junsik
,
Kim, Junsub
,
Lim, Hyungsoo
,
Bang, Je Sung
,
Seo, Jeong Min
,
Sohn, Jeong Lak
,
Lee, Jungho
DOI: 10.1115/1.4036882Publisher: The American Society of Mechanical Engineers (ASME)
Abstract: Effusion cooling is one of the attractive methods for next generation high-efficient gas turbine which has a very hot gas temperature above 1,600oC. For higher effectiveness of the air cooling, the air-cooled flow through effusion-holes does not penetrate into the mainstream flow but still remains within freestream boundary layer. So the air-cooled surface temperature maintains at relatively lower than film cooling. Effusion cooling is generally known as operating in small effusion-hole size which is less than 0.2 mm. This study is intended to examine optimum effusion-hole size of the microscale effusion cooling through flow visualization. The air flow through effusion-holes is visualized using an oil atomizer, a DSPP laser-sheet illumination, and a high-speed CCD imaging. The visualized results show flow patterns and characteristics with different blowing ratio, BR = ρcUc / ρ∞U∞, (BR = 0.17 and 0.53) and effusion-hole size (D = 0.2 mm, 0.5 mm and 1.0 mm). The flow visualization condition is fixed at the mainstream Reynolds number of 10,000 and hole-to-hole spacing of 4 (S/D = 4). For larger effusion-hole of 1.0 mm [(a) and (b)], the effusion flow can penetrate into boundary layer which exhibits a film cooling. However the effusion flow is observed to be remained within boundary layer which shows an effusion cooling for smaller effusion-hole of 0.2 mm [(e) and (f)]. In case of (c) and (d), a series of vortical structure is also observed to be within the boundary layer along the effusion flat plate. Note that the effusion-hole size of 0.5 mm can be a candidate for making effusion cooling possible. [This work was supported by National Research Council of Science and Technology (NST) grant funded by the Ministry of Science, ICT and Future Planning, Korea (Grant No. KIMM-NK203B).]
|
Collections
Show full item record
| contributor author | Lee, Junsik | |
| contributor author | Kim, Junsub | |
| contributor author | Lim, Hyungsoo | |
| contributor author | Bang, Je Sung | |
| contributor author | Seo, Jeong Min | |
| contributor author | Sohn, Jeong Lak | |
| contributor author | Lee, Jungho | |
| date accessioned | 2017-11-25T07:16:55Z | |
| date available | 2017-11-25T07:16:55Z | |
| date copyright | 2017/5/6 | |
| date issued | 2017 | |
| identifier issn | 0022-1481 | |
| identifier other | ht_139_08_080905.pdf | |
| identifier uri | http://138.201.223.254:8080/yetl1/handle/yetl/4234289 | |
| description abstract | Effusion cooling is one of the attractive methods for next generation high-efficient gas turbine which has a very hot gas temperature above 1,600oC. For higher effectiveness of the air cooling, the air-cooled flow through effusion-holes does not penetrate into the mainstream flow but still remains within freestream boundary layer. So the air-cooled surface temperature maintains at relatively lower than film cooling. Effusion cooling is generally known as operating in small effusion-hole size which is less than 0.2 mm. This study is intended to examine optimum effusion-hole size of the microscale effusion cooling through flow visualization. The air flow through effusion-holes is visualized using an oil atomizer, a DSPP laser-sheet illumination, and a high-speed CCD imaging. The visualized results show flow patterns and characteristics with different blowing ratio, BR = ρcUc / ρ∞U∞, (BR = 0.17 and 0.53) and effusion-hole size (D = 0.2 mm, 0.5 mm and 1.0 mm). The flow visualization condition is fixed at the mainstream Reynolds number of 10,000 and hole-to-hole spacing of 4 (S/D = 4). For larger effusion-hole of 1.0 mm [(a) and (b)], the effusion flow can penetrate into boundary layer which exhibits a film cooling. However the effusion flow is observed to be remained within boundary layer which shows an effusion cooling for smaller effusion-hole of 0.2 mm [(e) and (f)]. In case of (c) and (d), a series of vortical structure is also observed to be within the boundary layer along the effusion flat plate. Note that the effusion-hole size of 0.5 mm can be a candidate for making effusion cooling possible. [This work was supported by National Research Council of Science and Technology (NST) grant funded by the Ministry of Science, ICT and Future Planning, Korea (Grant No. KIMM-NK203B).] | |
| publisher | The American Society of Mechanical Engineers (ASME) | |
| title | Numerical Simulation of Evaporating Two-Phase Flow in a High-Aspect-Ratio Microchannel with Bends | |
| type | Journal Paper | |
| journal volume | 139 | |
| journal issue | 8 | |
| journal title | Journal of Heat Transfer | |
| identifier doi | 10.1115/1.4036882 | |
| journal fristpage | 80905 | |
| journal lastpage | 080905-6 | |
| tree | Journal of Heat Transfer:;2017:;volume( 139 ):;issue: 008 | |
| contenttype | Fulltext |