Boundary layer investigation in front of a blunt body in a subsonic air plasma flow by emission spectroscopic means

Author(s):  
Michael Winter ◽  
Monika Auweter-Kurtz
1997 ◽  
Author(s):  
M. Winter ◽  
M. Auweter-Kurtz ◽  
H. Kurtz ◽  
M. Winter ◽  
M. Auweter-Kurtz ◽  
...  

2019 ◽  
Vol 67 (2) ◽  
pp. 42-48
Author(s):  
Mayuko Tanaka ◽  
Kazuhiko Yamada ◽  
Yusuke Takahashi ◽  
Minghao Yu ◽  
Asei Tezuka

JETP Letters ◽  
2004 ◽  
Vol 79 (8) ◽  
pp. 368-371 ◽  
Author(s):  
S. P. Savin ◽  
L. M. Zelenyi ◽  
E. Amata ◽  
J. Buechner ◽  
J. Blecki ◽  
...  

1960 ◽  
Vol 27 (2) ◽  
pp. 223-229 ◽  
Author(s):  
M. V. Morkovin

For the purposes of assessing the magnitude of flow disturbances which would affect conditions on a blunt nose of a body moving at supersonic speeds, the detached shock is approximated by a purely normal shock. The disturbances downstream of the shock are expressed in terms of the “free-stream” disturbances by considering sinusoidal fluctuations. Pressure fluctuations generated by interactions of entropy-temperature disturbances with the normal shock may be considerable at high Mach numbers, but their effect on the transition of a laminar boundary layer to a turbulent one is a matter of speculation. However, conjectures that reflections of such pressure waves between the body and the shock wave might lead to high resonant amplifications are definitely disproved.


1975 ◽  
Vol 72 (1) ◽  
pp. 49-65 ◽  
Author(s):  
K. C. Wang

This paper investigates the three-dimensional laminar boundary layer over a blunt body (a prolate spheroid) at low incidence and with reversed flow. Results reflecting the general characteristics of such a problem are presented. More significant are the features relating to the circumferential flow reversal. Some of these features confirm our early hypotheses concerning the existence of a reversed region ahead of separation and the role of the zero-cfθ line in the general context of separation in three dimensions. Other features are unexpected, including the distribution of cfμ and the shape of the separation line. Here cfθ and cfμ denote, respectively, the circumferential and meridional components of the skin friction.


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