The Dispersion Rule of Fragments about the Asymmetric Shell
In order to obtain the dispersion rule of fragments about the asymmetric shell subjected to internal blast loading, two different cross section structures, concave-shaped and convex-shaped, were carried out by experimental and numerical methods. The simulation results well coincided with the experim...
Main Authors: | , , , , |
---|---|
Format: | Article |
Language: | English |
Published: |
Hindawi Limited
2017-01-01
|
Series: | Shock and Vibration |
Online Access: | http://dx.doi.org/10.1155/2017/9810978 |
id |
doaj-1d4e3e75bd7744bba3efdeb421f8f6cd |
---|---|
record_format |
Article |
spelling |
doaj-1d4e3e75bd7744bba3efdeb421f8f6cd2020-11-24T23:43:38ZengHindawi LimitedShock and Vibration1070-96221875-92032017-01-01201710.1155/2017/98109789810978The Dispersion Rule of Fragments about the Asymmetric ShellLiangliang Ding0Zhenduo Li1Minzu Liang2Xiangyu Li3Fangyun Lu4College of Science, National University of Defense Technology, Changsha, Hunan 410073, ChinaCollege of Science, National University of Defense Technology, Changsha, Hunan 410073, ChinaCollege of Science, National University of Defense Technology, Changsha, Hunan 410073, ChinaCollege of Science, National University of Defense Technology, Changsha, Hunan 410073, ChinaCollege of Science, National University of Defense Technology, Changsha, Hunan 410073, ChinaIn order to obtain the dispersion rule of fragments about the asymmetric shell subjected to internal blast loading, two different cross section structures, concave-shaped and convex-shaped, were carried out by experimental and numerical methods. The simulation results well coincided with the experimental results, and the spatial distribution and fragment velocity were obtained. The optimal curvatures for the different concave structures changed from 4r to 6r (r represents the charge radius), as the central angle of concave structure changed from 90° to 120°. However, the optimal curvature changed weakly when the central angle of concave structure was larger than 120°. In addition, a formula which can rapidly predict the projection angle range was fitted for the convex structure. The conclusions can provide a reference for concave-shaped and convex-shaped structures to achieve a higher effectiveness of fragments.http://dx.doi.org/10.1155/2017/9810978 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Liangliang Ding Zhenduo Li Minzu Liang Xiangyu Li Fangyun Lu |
spellingShingle |
Liangliang Ding Zhenduo Li Minzu Liang Xiangyu Li Fangyun Lu The Dispersion Rule of Fragments about the Asymmetric Shell Shock and Vibration |
author_facet |
Liangliang Ding Zhenduo Li Minzu Liang Xiangyu Li Fangyun Lu |
author_sort |
Liangliang Ding |
title |
The Dispersion Rule of Fragments about the Asymmetric Shell |
title_short |
The Dispersion Rule of Fragments about the Asymmetric Shell |
title_full |
The Dispersion Rule of Fragments about the Asymmetric Shell |
title_fullStr |
The Dispersion Rule of Fragments about the Asymmetric Shell |
title_full_unstemmed |
The Dispersion Rule of Fragments about the Asymmetric Shell |
title_sort |
dispersion rule of fragments about the asymmetric shell |
publisher |
Hindawi Limited |
series |
Shock and Vibration |
issn |
1070-9622 1875-9203 |
publishDate |
2017-01-01 |
description |
In order to obtain the dispersion rule of fragments about the asymmetric shell subjected to internal blast loading, two different cross section structures, concave-shaped and convex-shaped, were carried out by experimental and numerical methods. The simulation results well coincided with the experimental results, and the spatial distribution and fragment velocity were obtained. The optimal curvatures for the different concave structures changed from 4r to 6r (r represents the charge radius), as the central angle of concave structure changed from 90° to 120°. However, the optimal curvature changed weakly when the central angle of concave structure was larger than 120°. In addition, a formula which can rapidly predict the projection angle range was fitted for the convex structure. The conclusions can provide a reference for concave-shaped and convex-shaped structures to achieve a higher effectiveness of fragments. |
url |
http://dx.doi.org/10.1155/2017/9810978 |
work_keys_str_mv |
AT liangliangding thedispersionruleoffragmentsabouttheasymmetricshell AT zhenduoli thedispersionruleoffragmentsabouttheasymmetricshell AT minzuliang thedispersionruleoffragmentsabouttheasymmetricshell AT xiangyuli thedispersionruleoffragmentsabouttheasymmetricshell AT fangyunlu thedispersionruleoffragmentsabouttheasymmetricshell AT liangliangding dispersionruleoffragmentsabouttheasymmetricshell AT zhenduoli dispersionruleoffragmentsabouttheasymmetricshell AT minzuliang dispersionruleoffragmentsabouttheasymmetricshell AT xiangyuli dispersionruleoffragmentsabouttheasymmetricshell AT fangyunlu dispersionruleoffragmentsabouttheasymmetricshell |
_version_ |
1725500876018155520 |