Large-Eddy Simulation of Non-equilibrium Plasma-Assisted Combustion in Supersonic Flow

2008 ◽  
Author(s):  
Kenji Miki ◽  
Joseph Schulz ◽  
Suresh Menon
Keyword(s):  
Supersonic Flow ◽  
Large Eddy Simulation ◽  
Plasma Assisted Combustion ◽  
Equilibrium Plasma ◽  
Eddy Simulation ◽  
Large Eddy ◽  
Non Equilibrium

An improved dynamic non-equilibrium wall-model for large eddy simulation

2014 ◽  
Vol 26 (1) ◽  
pp. 015108 ◽  
Author(s):  
George Ilhwan Park ◽  
Parviz Moin
Keyword(s):  
Large Eddy Simulation ◽  
Wall Model ◽  
Eddy Simulation ◽  
Large Eddy ◽  
Non Equilibrium

Large Eddy Simulation of Film Cooling over a Flat Plate in Supersonic flow

2020 ◽  
pp. 1-29
Author(s):  
Hitesh Sharma ◽  
Dushyant Singh ◽  
Ashutosh Kumar Singh
Keyword(s):  
Heat Transfer ◽  
Supersonic Flow ◽  
Large Eddy Simulation ◽  
Flat Plate ◽  
Film Cooling ◽  
Cooling Effectiveness ◽  
Potential Core ◽  
Film Cooling Effectiveness ◽  
Eddy Simulation ◽  
Large Eddy

Abstract In the present work, Large Eddy Simulation (LES) was performed to access the film cooling performance in the supersonic flow over a flat plate with a perpendicular slot injection configuration. The study was carried out for three mainstream Mach No.; Mα = 1.2, 2.67, 3.3 and three coolant stream Mach No.; 0.05, 0.1, 0.15. In supersonic flow, temperature rise inside the boundary layer is a major issue considering it causes high rates of heat transfer to the coolant film. To select a suitable LES Sub-Grid Scale (SGS) model, LES results obtained from the present study using the LES Sub-Grid Scale (SGS) models such as Smagorinky- Lilly, Wale, and WMLES models were compared with DNS results available for flow and heat transfer. The parametric study showed that the higher mainstream Mach No. caused increased wall temperature and reduced effectiveness. The film cooling effectiveness appeared to reduce almost by 10% when the mainstream Mach No. is increased from 1.2 to 2.67, however, no apparent difference was observed in effectiveness between the mainstream Mach No. 2.67 and 3.3. It was found that doubling and tripling the coolant stream Mach No. from 0.05 to 0.1 and 0.15, the length of potential core region also doubled and tripled respectively from 4 X/S to 8 X/S and 13 X/S and hence significant improvement in the film cooling effectiveness was observed.

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