Propagation of shock waves in polydisperse gas suspensions

1993 ◽  
Vol 34 (2) ◽  
pp. 173-179 ◽  
Author(s):  
A. G. Kutushev ◽  
S. P. Rodionov
Keyword(s):  
1991 ◽  
Vol 27 (2) ◽  
pp. 223-231 ◽  
Author(s):  
V. M. Boiko ◽  
A. N. Papyrin ◽  
S. V. Poplavskii

KSME Journal ◽  
1988 ◽  
Vol 2 (1) ◽  
pp. 35-43 ◽  
Author(s):  
Y. Martsiano ◽  
G. Ben-Dor ◽  
O. Igra

AIAA Journal ◽  
1995 ◽  
Vol 33 (5) ◽  
pp. 953-955 ◽  
Author(s):  
F. Aizik ◽  
G. Ben-Dor ◽  
T. Elperin ◽  
O. Igra ◽  
M. Mond ◽  
...  

1996 ◽  
Vol 49 (10S) ◽  
pp. S141-S146 ◽  
Author(s):  
G. Ben-Dor

A review of our original article [1] is given. It describes the state-of-the art of the subject of the propagation and attenuation of planar shock waves in dust-gas suspensions. In addition, it includes a brief description of the Dust Entrainment Phenomenon. This relatively new subject in the general area of Dusty Shock Wave has been getting more and more attention in the past few years.


1989 ◽  
Vol 25 (2) ◽  
pp. 193-199 ◽  
Author(s):  
V. M. Boiko ◽  
V. V. Lotov ◽  
A. N. Papyrin

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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