scholarly journals Overdriven-detonation states produced by spherically diverging waves

2020 ◽  
Author(s):  
Matthew Biss ◽  
Mark Lieber ◽  
Michael Martinez
2021 ◽  
Vol 46 (4) ◽  
pp. 679-679
Author(s):  
Yakun Liu ◽  
Jianping Yin ◽  
Zhijun Wang

2003 ◽  
Author(s):  
Masahiko Otsuka ◽  
Hideyuki Morimoto ◽  
Shirou Nagano ◽  
Eiji Hida ◽  
Kenji Kuroki ◽  
...  

2004 ◽  
Author(s):  
Yamato Matsui ◽  
Hideki Hamashima ◽  
Shigeru Itoh

2000 ◽  
Vol 20 (79) ◽  
pp. 303-308_1
Author(s):  
A.Koichi HAYASHI ◽  
Yasunari MIKUTSU ◽  
Norio ARAKI

2019 ◽  
Vol 36 (4) ◽  
pp. 391-399
Author(s):  
Gui-yang Xu ◽  
Chun-guang Wang ◽  
Shao-qing Hu ◽  
Jian-Liang Gong ◽  
Zhe Deng

Abstract The time error of detonation acoustic in process of detonation formation and propagation in a multi-cycle gas-liquid two-phase pulsed detonation engine is experimentally investigated. Results from the tests show that before the detonation wave escapes through the open-end of PDE tube, the maximum average arrival time error of detonation acoustic is achieved in the process of overdriven detonation. After detonation wave exists of PDE tube, arrival time error at 0 deg is greater than the other directivity angles in all distances and increases dramatically first and then almost stays at a certain value. The filling fraction has a major impact on the time error of detonation acoustic. With filling fraction increasing, there are increases in arrival time error and interval time error. Arrival time error with the highest filling fraction at 30 deg is much greater than other filling fraction. The convergent nozzle exhibits a marked suppression in the time error of detonation acoustic, where the maximum reductions of 62.02 percent and 56.13 percent are obtained in arrival time error and interval time error respectively.


1970 ◽  
Vol 43 (2) ◽  
pp. 399-406 ◽  
Author(s):  
C. R. Wilson ◽  
D. L. Turcotte

A similarity solution has been obtained for a radiation-driven shock wave. Radiation propagating radially inwards is completely absorbed in the shock layer of a spherical, expanding shock wave. For a strong shock wave and a constant power input a similarity solution is obtained. It is found that the radial position of the shock wave rs ∼ t⅗. The shock wave propagates as an overdriven detonation. The jump conditions and complete flow field are obtained.


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