scholarly journals Supersonic airplane engine jet influence on the intensity of tail shock wave of sonic boom waveform

2019 ◽  
Vol 1404 ◽  
pp. 012126
Author(s):  
V F Volkov
2003 ◽  
Vol 114 (4) ◽  
pp. 1758-1771 ◽  
Author(s):  
Régis Marchiano ◽  
François Coulouvrat ◽  
Richard Grenon

1974 ◽  
Vol 11 (12) ◽  
pp. 745-751
Author(s):  
G. T. Haglund ◽  
E. J. Kane
Keyword(s):  

2008 ◽  
Vol 123 (5) ◽  
pp. 3695-3695
Author(s):  
Lili Ganjehi ◽  
François Coulouvrat ◽  
Jean‐Louis Thomas ◽  
Régis Marchiano

Author(s):  
Constantin Sandu ◽  
Radu-Constantin Sandu ◽  
Cristian-Teodor Olariu

Author(s):  
R. Sharma ◽  
B.L. Ramakrishna ◽  
N.N. Thadhani ◽  
D. Hianes ◽  
Z. Iqbal

After materials with superconducting temperatures higher than liquid nitrogen have been prepared, more emphasis has been on increasing the current densities (Jc) of high Tc superconductors than finding new materials with higher transition temperatures. Different processing techniques i.e thin films, shock wave processing, neutron radiation etc. have been applied in order to increase Jc. Microstructural studies of compounds thus prepared have shown either a decrease in gram boundaries that act as weak-links or increase in defect structure that act as flux-pinning centers. We have studied shock wave synthesized Tl-Ba-Cu-O and shock wave processed Y-123 superconductors with somewhat different properties compared to those prepared by solid-state reaction. Here we report the defect structures observed in the shock-processed Y-124 superconductors.


Author(s):  
M.A. Mogilevsky ◽  
L.S. Bushnev

Single crystals of Al were loaded by 15 to 40 GPa shock waves at 77 K with a pulse duration of 1.0 to 0.5 μs and a residual deformation of ∼1%. The analysis of deformation structure peculiarities allows the deformation history to be re-established.After a 20 to 40 GPa loading the dislocation density in the recovered samples was about 1010 cm-2. By measuring the thickness of the 40 GPa shock front in Al, a plastic deformation velocity of 1.07 x 108 s-1 is obtained, from where the moving dislocation density at the front is 7 x 1010 cm-2. A very small part of dislocations moves during the whole time of compression, i.e. a total dislocation density at the front must be in excess of this value by one or two orders. Consequently, due to extremely high stresses, at the front there exists a very unstable structure which is rearranged later with a noticeable decrease in dislocation density.


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