Numerical Simulation of Shock Wave Interaction Effects on Supersonic Mixing Layer Growth

2001 ◽  
pp. 217-228 ◽  
Author(s):  
U. Wepler ◽  
Ch. Huhn ◽  
W. Koschel
Keyword(s):  
Numerical Simulation ◽  
Shock Wave ◽  
Mixing Layer ◽  
Wave Interaction ◽  
Interaction Effects ◽  
Layer Growth ◽  
Shock Wave Interaction ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer

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.

scholarly journals Diffusion-Flame Ignition by Shock-Wave Impingement on a Hydrogen–Air Supersonic Mixing Layer

2017 ◽  
Vol 33 (1) ◽  
pp. 256-263 ◽  
Author(s):  
César Huete ◽  
Antonio L. Sánchez ◽  
Forman A. Williams
Keyword(s):  
Shock Wave ◽  
Diffusion Flame ◽  
Mixing Layer ◽  
Supersonic Mixing ◽  
Flame Ignition ◽  
Supersonic Mixing Layer

Direct numerical simulation of fine flow structures of subsonic-supersonic mixing layer

2019 ◽  
Vol 95 ◽  
pp. 105431 ◽  
Author(s):  
Liu Yang ◽  
Ma Dong ◽  
Fu Benshuai ◽  
Li Qiang ◽  
Zhang Chenxi
Keyword(s):  
Numerical Simulation ◽  
Direct Numerical Simulation ◽  
Mixing Layer ◽  
Flow Structures ◽  
Supersonic Mixing ◽  
Supersonic Mixing Layer

Numerical simulation of shock wave interaction with powder layers

Shock Waves ◽  
1992 ◽  
pp. 563-568 ◽  
Author(s):  
H. Sakakita ◽  
A. K. Hayashi ◽  
A. I. Ivandaev
Keyword(s):  
Numerical Simulation ◽  
Shock Wave ◽  
Wave Interaction ◽  
Shock Wave Interaction

Numerical Simulation of a Three-Dimensional Flame/Shock Wave Interaction

AIAA Journal ◽  
2000 ◽  
Vol 38 (5) ◽  
pp. 745-754 ◽  
Author(s):  
Christopher J. Roy ◽  
Jack R. Edwards
Keyword(s):  
Numerical Simulation ◽  
Shock Wave ◽  
Three Dimensional ◽  
Wave Interaction ◽  
Shock Wave Interaction
Sign in / Sign up

Export Citation Format

Share Document