Effects of sidewall disturbances on the supersonic mixing layer

1992 ◽  
Vol 8 (1) ◽  
pp. 249-251 ◽  
Author(s):  
N. T. Clemens ◽  
M. G. Mungal
Keyword(s):  
Mixing Layer ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer

A review on enhanced mixing methods in supersonic mixing layer flows

2018 ◽  
Vol 152 ◽  
pp. 310-324 ◽  
Author(s):  
Jianguo Tan ◽  
Dongdong Zhang ◽  
Liang Lv
Keyword(s):  
Mixing Layer ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer ◽  
Mixing Layer Flows

A thermo-chemical exploration of a two-dimensional reacting supersonic mixing layer

1997 ◽  
Vol 9 (11) ◽  
pp. 3513-3522 ◽  
Author(s):  
Debasis Chakraborty ◽  
H. V. Nagaraj Upadhyaya ◽  
P. J. Paul ◽  
H. S. Mukunda
Keyword(s):  
Mixing Layer ◽  
Two Dimensional ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer

On the cavity-actuated supersonic mixing layer downstream a thick splitter plate

2020 ◽  
Vol 32 (9) ◽  
pp. 096102 ◽  
Author(s):  
Jianguo Tan ◽  
Hao Li ◽  
Bernd R. Noack
Keyword(s):  
Mixing Layer ◽  
Splitter Plate ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer

scholarly journals A LES Study on Passive Mixing in Supersonic Shear Layer Flows Considering Effects of Baffle Configuration

2014 ◽  
Vol 6 ◽  
pp. 836146 ◽  
Author(s):  
Ren Zhao-Xin ◽  
Wang Bing
Keyword(s):  
Pressure Loss ◽  
Total Pressure ◽  
Large Scale ◽  
Mixing Layer ◽  
Total Pressure Loss ◽  
Mixing Efficiency ◽  
Mixing Enhancement ◽  
Supersonic Mixing ◽  
Passive Mixing ◽  
Supersonic Mixing Layer

Under the background of dual combustor ramjet (DCR), a numerical investigation of supersonic mixing layer was launched, focused on the mixing enhancement method of applying baffles with different geometric configurations. Large eddy simulation with high order schemes, containing a fifth-order hybrid WENO compact scheme for the convective flux and sixth-order compact one for the viscous flux, was utilized to numerically study the development of the supersonic mixing layer. The supersonic cavity flow was simulated and the cavity configuration could influence the mixing characteristics, since the impingement process of large scale structures formed inside the cavity could raise the vorticity and promote the mixing. The effect of baffle's configurations on the mixing process was analyzed by comparing the flow properties, mixing efficiency, and total pressure loss. The baffle could induce large scale vortexes, promote the mixing layer to lose its stability easily, and then lead to the mixing efficiency enhancement. However, the baffle could increase the total pressure loss. The present investigation could provide guidance for applying new passive mixing enhancement methods for the supersonic mixing.

Diffusion-flame ignition by shock-wave impingement on a supersonic mixing layer

2015 ◽  
Vol 784 ◽  
pp. 74-108 ◽  
Author(s):  
César Huete ◽  
Antonio L. Sánchez ◽  
Forman A. Williams ◽  
Javier Urzay
Keyword(s):  
Shock Wave ◽  
Chemical Reaction ◽  
Diffusion Flame ◽  
Mixing Layer ◽  
Damkohler Number ◽  
Damköhler Number ◽  
Supersonic Mixing ◽  
Post Shock ◽  
Supersonic Mixing Layer ◽  
Ignition Kernel

Ignition in a supersonic mixing layer interacting with an oblique shock wave is investigated analytically and numerically under conditions such that the post-shock flow remains supersonic. The study requires consideration of the structure of the post-shock ignition kernel that is found to exist around the point of maximum temperature, which may be located either near the edge of the mixing layer or in its interior, depending on the profiles of the fuel concentration, temperature and Mach number across the mixing layer. The ignition kernel displays a balance between the rates of chemical reaction and of post-shock flow expansion, including the acoustic interactions of the chemical heat release with the shock wave, leading to increased front curvature. The analysis, which adopts a one-step chemistry model with large activation energy, indicates that ignition develops as a fold bifurcation, the turning point in the diagram of the peak perturbation induced by the chemical reaction as a function of the Damköhler number providing the critical conditions for ignition. While an explicit formula for the critical Damköhler number for ignition is derived when ignition occurs in the interior of the mixing layer, under which condition the ignition kernel is narrow in the streamwise direction, numerical integration is required for determining ignition when it occurs at the edge, under which condition the kernel is no longer slender. Subsequent to ignition, for the Arrhenius chemistry addressed, the lead shock will rapidly be transformed into a thin detonation on the fuel side of the ignition kernel, and, under suitable conditions, a deflagration may extend far downstream, along with the diffusion flame that must separate the rich and lean reaction products. The results can be helpful in describing supersonic combustion for high-speed propulsion.

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