JAST. Vol. 9, No. 1, pp 13-26
© Iranian Aerospace Society, Winter - Spring 2012
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Journal ofA S T
Aerospace Science and TechnologyNomenclature
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An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
M.R. Salimi
1, M. Taeibi-Rahni
2, M. Ramezanizadeh
3, and R. Farhadi-Azar
4A new design concept is introduced to control the near-wall integration between the !""# "# ! ! # ! " $ -% "# "" " & ( "" (!"#! "$! # )#((!!!" $ &#" $(! # " #"&!! $! !#!! # " & " using the Reynolds-averaged Navier-Stokes equations closed by the v2f - k w turbulence &$$(!*!+, ./++#"
Keywords0 1 3 # 4 & 5# 6" 7# 8 9#2f - k w Turbulence Model
1. Ph.D Student, Dep't. of Aerospace Eng., Sharif University of #&#=0>?@BC 2. Professor, Dep't. of Aerospace Eng., Sharif University of
Technol-ogy, Tehran, Iran.
?) F G3" )H# K"O )" Eng., Shahid Sattari Aeronautical University of Science & #&#=0WWC . 9 4# K"O )" = # 9 6
Technology, Tehran, Iran.
1 Introduction
' M.R. Salimi, M. Taeibi-Rahni, M. Ramezanizadeh, and R. Farhadi-Azar
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D An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
5 Physical Domain and Boundary Conditions * 4 -+#
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= An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
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Table 2. Number of grid points used in the main jet channel.
Table 3. Number of grid points used in the upstream jet channel.
$" cooling effectiveness.
Q? M.R. Salimi, M. Taeibi-Rahni, M. Ramezanizadeh, and R. Farhadi-Azar
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X/D=3.0.
X/D=5.0.
X/D=8.0.
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provided by different turbulence models at Z/D=0.0 and X/D=5.0.
Q An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
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Figure 7. Stream lines and pressure contours at Z/D=0.0.
Figure 8. Film cooling effectiveness contours **+
QQ M.R. Salimi, M. Taeibi-Rahni, M. Ramezanizadeh, and R. Farhadi-Azar
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Q; An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
4
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X/D=5
Figure 12. Local temperature distribution at different X/D positions.
X/D=3
Q' M.R. Salimi, M. Taeibi-Rahni, M. Ramezanizadeh, and R. Farhadi-Azar
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7.3 Effects of Jets’ Area Ratio
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Q> An Innovation in Film Cooling of Gas Turbine Blades Applying an Upstream Jet
Figure 16. Rise in span-wise averaged effectiveness for three differ-ent area ratios.
7.4 Effects on the Skin Friction Drag (
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8 Conclusions
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9 References
O 5U L/4$ 7H H 55 <7 8<@5+":) G International Journal of Heat and Mass Transfer8'CUQQQ4Q;>Q??;
Q 7/@ * E4 E G H 5"@ H<G 5 International Journal of Heat and
Fluid Flow8Q=U4DQ??K
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> $ < @4/ <: Z $@ H5G < 5Heat and Mass Transfer. J 8''UK=K=4==KQ??K
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8:<LInternational Journal
of Rotating Machinery 8 ? U > ;'>4 ;>'Q??'
= L Z B 5O U @ < G 5 G H:)))5 5International Journal of Heat and Mass Transfer8'=U>4C==4=;KQ??C
? EO@*G((<$ <H5")+ <International Journal of Heat and Fluid Flow8QKU>=QQ4=;Q??D
<78<4 @5+":)G International Journal of Heat and Mass Transfer 8'CUQQQ4Q;>Q??;
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