Analytical prediction of the reflected-diffracted shock wave shape in the interaction of a regular reflection with an expansive corner

1994 ◽  
Vol 14 (5) ◽  
pp. 229-239 ◽  
Author(s):  
H Li ◽  
G Ben-Dor ◽  
Z Y Han
Fluids ◽  
2021 ◽  
Vol 6 (9) ◽  
pp. 305
Author(s):  
Mikhail V. Chernyshov ◽  
Karina E. Savelova ◽  
Anna S. Kapralova

In this study, we obtain the comparative analysis of methods of quick approximate analytical prediction of Mach shock height in planar steady supersonic flows (for example, in supersonic jet flow and in narrowing channel between two wedges), that are developed since the 1980s and being actively modernized now. A new analytical model based on flow averaging downstream curved Mach shock is proposed, which seems more accurate than preceding models, comparing with numerical and experimental data.


2020 ◽  
Vol 899 ◽  
Author(s):  
Longsheng Xue ◽  
Ferry F. J. Schrijer ◽  
Bas W. van Oudheusden ◽  
Chengpeng Wang ◽  
Zhiwei Shi ◽  
...  

Abstract


Author(s):  
Fedor V. Potemkin ◽  
Evgeniy I. Mareev ◽  
Vjacheslav M. Gordienko ◽  
Aleksey A. Podshivalov

1983 ◽  
Vol 18 (2) ◽  
pp. 243-247
Author(s):  
V. I. Bogatko ◽  
G. A. Kolton

2017 ◽  
Vol 813 ◽  
pp. 70-84 ◽  
Author(s):  
V. Soni ◽  
A. Hadjadj ◽  
A. Chaudhuri ◽  
G. Ben-Dor

Numerical simulations were conducted to understand the different wave configurations associated with the shock-wave reflections over double-concave cylindrical surfaces. The reflectors were generated computationally by changing different geometrical parameters, such as the radii of curvature and the initial wedge angles. The incident-shock-wave Mach number was varied such as to cover subsonic, transonic and supersonic regimes of the flows induced by the incident shock. The study revealed a number of interesting wave features starting from the early stage of the shock interaction and transition to transitioned regular reflection (TRR) over the first concave surface, followed by complex shock reflections over the second one. Two new shock bifurcations have been found over the second wedge reflector, depending on the velocity of the additional wave that appears during the TRR over the first wedge reflector. Unlike the first reflector, the transition from a single-triple-point wave configuration (STP) to a double-triple-point wave configuration (DTP) and back occurred several times on the second reflector, indicating that the flow was capable of retaining the memory of the past events over the entire process.


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