Corrections to the Rankine-Hugoniot conditions for curved shock waves

2014 ◽  
Author(s):  
Carlo Lancellotti ◽  
Yubei Yue
Shock Waves ◽  
2017 ◽  
Vol 27 (5) ◽  
pp. 699-720 ◽  
Author(s):  
S. Mölder

1947 ◽  
Vol 26 (1-4) ◽  
pp. 62-68 ◽  
Author(s):  
T. Y. Thomas

Fluids ◽  
2021 ◽  
Vol 6 (9) ◽  
pp. 303
Author(s):  
Beric Skews

Studies of shock-vortex interactions in the past have predominantly been numerical, with a number of idealizations such as assuming an isolated vortex and a plane shock wave. In the present case the vortex is generated from flow separation at a corner. A shear layer results which wraps up into a spiral vortex. The flow is impulsively initiated by the diffraction of a shock wave over the edge. The strength of the shock determines the nature of the flow at the corner and that induced behind the diffracted wave. A wide variety of cases are considered using different experimental arrangements such as having two independent shock waves arriving at the corner at different times, to reflecting the diffracting wave off different surfaces back into the vortex, and to examining the flow around bends where the reflection off the far wall reflects back onto the vortex. The majority of studies have shown that the vortex normally retains its integrity after shock transit. Some studies with curved shock waves and numerous traverses have shown evidence of vortex breakup and the development of turbulent patches in the flow, as well as significant vortex stretching. Depending on the direction of approach of the shock wave it refracts through the shear layer thereby changing the strength and direction of both. Of particular note is that the two diffracted waves which emerge from the vortex as the incident wave passes through interact with each other resulting in a pressure spike of considerable magnitude. An additional spike is also identified.


Sign in / Sign up

Export Citation Format

Share Document