Effects of cavity-induced mixing enhancement under oblique shock wave interference: Numerical study

Author(s):  
Zuo Qiuru ◽  
Yu Huanli ◽  
Dai Jian
Shock Waves ◽  
2008 ◽  
Vol 18 (3) ◽  
pp. 193-204 ◽  
Author(s):  
J. C. Huang ◽  
T. Y. Hsieh ◽  
J. Y. Yang ◽  
K. Takayama

1992 ◽  
Vol 27 (2) ◽  
pp. 196-201
Author(s):  
V. I. Vasil'ev ◽  
S. N. Zakotenko

A direct comparison is made for several occurrences of oblique shock-wave reflections between interferometric results obtained at the University of Toronto Institute for Aerospace Studies (UTIAS) 10 cm x 18 cm hyper­-velocity shock tube and numerical results obtained by using a current computational method for solving the Euler equations. Very good qualitative agreement is obtained for equilibrium and frozen flow fields except in small regions where the experiments were dominated by viscous flow. The quantitative agreement is very close in some cases but can be out by 10–15% in cases with non-equilibrium flow or viscous structures or both. Additional parametrized sequences of calculations are presented to assess the utility of the present numerical method in constructing the various reflection–transition lines for perfect inviscid flows in the shock-wave Mach number, wedge-angle ( M s , θ w )-plane, and the validity of the ‘boundary-layer defect’ theory.


1987 ◽  
Vol 177 ◽  
pp. 247-263 ◽  
Author(s):  
G. Degrez ◽  
C. H. Boccadoro ◽  
J. F. Wendt

An investigation of an oblique shock wave/laminar boundary layer interaction is presented. The Mach number was 2.15, the Reynolds number was 105 and the overall pressure ratio was 1.55. The interation has been demonstrated to be laminar and nominally two-dimensional. Experimental results include pressure distributions on the plate and single component laser-Doppler velocimetry velocity measurements both in the attached and separated regions.The numerical results have been obtained by solving the full compressible Navier-Stokes equations with the implicit approximate factorization algorithm by Beam & Warming (1980). Comparison with experimental data shows good agreement in terms of pressure distributions, positions of separation and reattachment and velocity profiles.


Author(s):  
Sunghun Lee ◽  
Myeongwon Lee ◽  
Jin Park ◽  
Hongjip Kim

Abstract The center body diffuser is one of supersonic diffuser that can simulate high-altitude environment. There is center-body structure inside the diffuser, and a complex fluid flow is occurred inside the diffuser because of the interaction of the CB structure with gas exhausted from the nozzle outlet. In this study, starting point and flow characteristics of diffuser were investigated according to changing the CB nose cone angle and the length of distance between nozzle and CB structure. The differences of the supersonic flow were compared through each parameter of CB distance and CB nose angle. First changed parameter was length between nozzle and CB. According to the length of distance between nozzle and CB, axial momentum was developed and oblique shock wave moved front of CB from end of CB nose cone. Also, when CB position was located on a certain length, starting point of CBD decreased. Next change parameter was angle of CB nose cone. According to the angle raised, angle of oblique shock wave was raised and radial momentum of supersonic diffuser developed. But, according to radial momentum of supersonic flow over certain angle, the starting pressure of CBD increased. Because axial momentum which isolated vacuum chamber from atmospheric pressure. Through these CFD analysis results, it was shown that angle and length of distance between nozzle and CB influent performance of CBD.


2002 ◽  
Vol 24 (3) ◽  
pp. 149-157 ◽  
Author(s):  
C. A. R. Pimentel ◽  
J. L. F. Azevedo ◽  
L.F. Figueira da Silva ◽  
B. Deshaies

2020 ◽  
Author(s):  
K. Yu. Arefyev ◽  
O. V. Guskov ◽  
A. N. Prokhorov ◽  
A. S. Saveliev ◽  
E. E. Son ◽  
...  

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