石英玻璃球撞击刚性壁的破碎过程

方继松 王珠 熊迅 郑宇轩 周风华

方继松, 王珠, 熊迅, 郑宇轩, 周风华. 石英玻璃球撞击刚性壁的破碎过程[J]. 高压物理学报, 2020, 34(1): 014101. doi: 10.11858/gywlxb.20190764
引用本文: 方继松, 王珠, 熊迅, 郑宇轩, 周风华. 石英玻璃球撞击刚性壁的破碎过程[J]. 高压物理学报, 2020, 34(1): 014101. doi: 10.11858/gywlxb.20190764
FANG Jisong, WANG Zhu, XIONG Xun, ZHENG Yuxuan, ZHOU Fenghua. Fragmentation Process of Quartz Glass Spheres Impacting Rigid Wall[J]. Chinese Journal of High Pressure Physics, 2020, 34(1): 014101. doi: 10.11858/gywlxb.20190764
Citation: FANG Jisong, WANG Zhu, XIONG Xun, ZHENG Yuxuan, ZHOU Fenghua. Fragmentation Process of Quartz Glass Spheres Impacting Rigid Wall[J]. Chinese Journal of High Pressure Physics, 2020, 34(1): 014101. doi: 10.11858/gywlxb.20190764

石英玻璃球撞击刚性壁的破碎过程

doi: 10.11858/gywlxb.20190764
基金项目: 国家自然科学基金(11390361)
详细信息
    作者简介:

    方继松(1993-),男,硕士研究生,主要从事冲击动力学研究. E-mail: 2633186318@qq.com

    通讯作者:

    周风华(1964-),男,博士,研究员,主要从事冲击动力学研究. E-mail: zhoufenghua@nbu.edu.cn

  • 中图分类号: O347

Fragmentation Process of Quartz Glass Spheres Impacting Rigid Wall

  • 摘要: 利用高速枪对石英玻璃球撞击刚性靶板进行了实验研究,分析了不同速度下球体的破碎过程和失效模式。当冲击速度低于临界破坏速度时,石英玻璃球以略低于原速从靶板回弹;当超过临界破坏速度时,球体呈现“压缩破碎区-表面剥落区-剪切破坏区”的破坏结构;进一步提高碰撞速度,剪切破坏区的扩展导致球体碎裂为若干“月牙状”的碎块;更高撞击速度下,石英玻璃球发生坍塌式破碎,在远离撞击端处产生层裂现象。利用离散元软件对球体的撞击破坏过程进行了模拟研究,球体在高速碰撞下的破碎可以分为弹性压缩、整体破碎和二次撞击3个阶段。球体碎裂前Hertz接触理论可以较好描述其撞击力,而破碎后的撞击力由于碎裂卸载远小于理论值,且偏差随冲击速度逐渐增加。

     

  • 图  实验装置示意图

    Figure  1.  Schematic of experimental device

    图  临界速度以下碰撞前(a)、后(b)球体形貌

    Figure  2.  Sphere before (a) and after (b) impact under critical velocity

    图  石英玻璃球撞击刚性壁典型的破碎过程

    Figure  3.  Typical fracture process of sphere impact rigid wall

    图  不同撞击速度下球体的破碎形貌

    Figure  4.  Shape of spheres under different impact velocities

    图  不同冲击速度下碎片回收形貌

    Figure  5.  Shape of the fragments at different impact velocities

    图  78 m/s冲击速度下石英玻璃球的破碎过程

    Figure  6.  Fragmentation process of quartz glass sphere at 78 m/s

    图  球体速度、所受载荷和内部裂纹随时间变化曲线

    Figure  7.  Sphere velocity, impact force and internal crack versus time

    图  不同冲击速度下球体速度-时间曲线

    Figure  8.  Velocity-time curves at different impact velocities

    图  不同冲击速度下球体所受载荷

    Figure  9.  Impact forces of spheres under different impact velocities

    图  10  模拟撞击力与Hertz接触理论对比

    Figure  10.  Comparison of simulated impact forces with Hertz contact theory

    表  1  石英玻璃离散元模型的主要微观参数

    Table  1.   Main microscopic parameters of discrete element mode of quartz glass

    Effective modulus of linear contact/GPaNormal to shear stiffness ratio of linear contactPorosityMinimum radius of particles/mmSize ratio of maximum and minimum particlesTensile strength of contact/MPaShear strength of contact/MPa
    552.90.20.11.5300600
    下载: 导出CSV

    表  2  石英玻璃在常态下的物理参数

    Table  2.   Physical properties of quartz glass under ambient condition

    MethodEquivalent density/(kg·m–3)Elastic modulus/GPaPoisson’s ratioCompressive strength/MPaTensile strength/MPaBending strength/MPaFracture toughness/(N·m–3/2)
    Manufacture provide2.20377.80.1708605067.00.78
    DEM numerical simulation2.20378.00.1727985067.40.85
    下载: 导出CSV
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出版历程
  • 收稿日期:  2019-04-23
  • 修回日期:  2019-05-15
  • 刊出日期:  2019-09-25

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