首页 | 官方网站   微博 | 高级检索  
     

定向断裂双孔爆破含缺陷介质裂纹扩展的动焦散试验
引用本文:王雁冰,商禹智,石震鑫,田秋实,王恒攀,张显裕. 定向断裂双孔爆破含缺陷介质裂纹扩展的动焦散试验[J]. 爆破, 2018, 35(1): 15-20,48. DOI: 10.3963/j.issn.1001-487X.2018.01.003
作者姓名:王雁冰  商禹智  石震鑫  田秋实  王恒攀  张显裕
作者单位:中国矿业大学(北京)力学与建筑工程学院,北京,100083;中国矿业大学(北京)力学与建筑工程学院,北京,100083;中国矿业大学(北京)力学与建筑工程学院,北京,100083;中国矿业大学(北京)力学与建筑工程学院,北京,100083;中国矿业大学(北京)力学与建筑工程学院,北京,100083;中国矿业大学(北京)力学与建筑工程学院,北京,100083
基金项目:中国博士后科学基金面上项目,国家留学基金建设高水平大学公派研究生项目
摘    要:利用爆炸加载数字激光动态焦散线试验系统,进行双孔爆破爆炸应力波作用下缺陷介质裂纹扩展试验。研究了含水平预制裂纹和竖直预制裂纹的介质裂纹扩展路径、速度、加速度和裂尖动态应力强度因子变化规律。试验结果表明:在爆炸应力波作用下,预制裂纹尖端起裂,并扩展。炸药爆炸后,主裂纹的扩展速度迅速达到峰值,之后开始振荡减小,其加速度呈现波浪起伏式的振荡变化。次裂纹起裂后速度增大至峰值,然后开始减小。主裂纹尖端的动态应力强度因子K_Ⅰ从峰值振荡减小,又振荡增加至第二个峰值,之后振荡减小。次裂纹尖端的动态应力强度因子K_Ⅰ达到最大时,次裂纹起裂,之后K_Ⅰ振荡减小。裂纹扩展的过程中K_Ⅱ基本都小于K_Ⅰ。

关 键 词:双孔爆破  缺陷介质  裂纹扩展  动焦散试验  动态应力强度因子

Dynamic Caustics Experiment on Crack Propagation in Defective Medium by Directional Breaking with Double Hole Blasting
WANG Yan-bing,SHANG Yu-zhi,SHI Zhen-xin,TIAN Qiu-shi,WANG Heng-Pan,ZHANG Xian-yu. Dynamic Caustics Experiment on Crack Propagation in Defective Medium by Directional Breaking with Double Hole Blasting[J]. Blasting, 2018, 35(1): 15-20,48. DOI: 10.3963/j.issn.1001-487X.2018.01.003
Authors:WANG Yan-bing  SHANG Yu-zhi  SHI Zhen-xin  TIAN Qiu-shi  WANG Heng-Pan  ZHANG Xian-yu
Abstract:The experimental system of explosive load digital laser dynamic caustics was used to study the propa-gation behavior of cracks under the effect of explosive stress waves of double holes explosion.Meanwhile,the path, velocity and acceleration of the propagation of cracks in a Polymethyl methacrylate(PMMA)medium were also stud-ied,including horizontal and vertical prefabricated cracks and the variation of dynamic stress intensity factor at the tip of the cracks.The experimental results show that the tip of the prefabricated cracks propagated under the effect of an explosive stress wave.After detonation,the velocity of the main crack rapidly peaked,then decreased in oscillation. After the secondary crack,its velocity peaked and then began to decrease.The dynamic stress intensity factor KⅠat the main crack's tip decreased from the peak value in oscillation,and increased to the second peak value,then de-crease in oscillation.When the dynamic stress intensity factor KⅠat the main crack's tip reached the maximum val-ue,the secondary crack initiated,and then KⅠdecreased in oscillation.In the process of crack propagation,the KⅡwas almost less than KⅠ.
Keywords:
本文献已被 CNKI 万方数据 等数据库收录!
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司    京ICP备09084417号-23

京公网安备 11010802026262号