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不同倾角充填节理对岩石爆破块度的影响

陶明 曹峥 赵瑞 刘玉龙 李夕兵

陶明, 曹峥, 赵瑞, 刘玉龙, 李夕兵. 不同倾角充填节理对岩石爆破块度的影响[J]. 爆炸与冲击. doi: 10.11883/bzycj-2024-0414
引用本文: 陶明, 曹峥, 赵瑞, 刘玉龙, 李夕兵. 不同倾角充填节理对岩石爆破块度的影响[J]. 爆炸与冲击. doi: 10.11883/bzycj-2024-0414
TAO Ming, CAO Zheng, ZHAO Rui, LIU Yulong, LI Xibing. Influence of filled joints with different inclination angles on rock blasting fragmentation[J]. Explosion And Shock Waves. doi: 10.11883/bzycj-2024-0414
Citation: TAO Ming, CAO Zheng, ZHAO Rui, LIU Yulong, LI Xibing. Influence of filled joints with different inclination angles on rock blasting fragmentation[J]. Explosion And Shock Waves. doi: 10.11883/bzycj-2024-0414

不同倾角充填节理对岩石爆破块度的影响

doi: 10.11883/bzycj-2024-0414
基金项目: 国家自然科学基金(12072376);
详细信息
    作者简介:

    陶 明(1983- ),男,博士,教授,mingtao@csu.edu.cn

    通讯作者:

    陶 明(1983- ),男,博士,教授,mingtao@csu.edu.cn

  • 中图分类号: P

Influence of filled joints with different inclination angles on rock blasting fragmentation

  • 摘要: 为了理解节理与爆炸应力波之间的相互作用,并优化节理岩体的爆破参数,通过试验与数值模拟相结合的方式研究不同节理倾角对爆破块度的影响:采用一组含有不同角度节理的混凝土模型试样开展爆破试验,在试样竖直孔中装填雷管并爆破,使用高速摄像机记录试样爆破破碎过程,观测起爆后不同时刻节理面的动态响应;利用图像处理方法进行爆破块度提取,分析节理倾角对爆破块度的影响;采用LS-DYNA有限元数值模拟获得应力波的传播过程以及应变场的演变过程。试验与数值计算结果表明:节理对爆破块度分布及应力波传播有显著影响,该影响主要源于爆炸应力波在节理处的反射,这与节理的变形特性有关;随着节理倾角增大,爆破块度先减小后增大,节理中的有效应力和峰值质点振动速度透射总体呈下降趋势,但在45°至60°之间回升,其中45°左右为爆破最有利条件。数值裂纹网络重建和图像处理结果表明,随着节理倾角的增加,试样中产生的垂直裂纹增加,水平裂纹有所减少。
  • 图  1  试样浇筑

    Figure  1.  Specimen concreting

    图  2  试验模型

    Figure  2.  Experimental model

    图  3  试样图

    Figure  3.  Photograph of the bar sample

    图  4  爆破试验示意图

    Figure  4.  Schematic of blasting experiment

    图  5  试样最终破坏情况

    Figure  5.  The final destruction of the samples

    图  6  内、外层爆破效果及岩体爆破块度分区示意图

    Figure  6.  Illustration of inner and outer blasting effects and partition of rock blasting fragmentation

    图  7  钻孔周围破坏过程高速照片

    Figure  7.  High-speed photographs of the destruction process around the borehole

    图  8  节理应变场演变(t = 250 μs, 375 μs, 500 μs, 625 μs, 750 μs, 875 μs)

    Figure  8.  Strain field evolution of joints(t = 250 μs, 375 μs, 500 μs, 625 μs,750 μs. 875 μs)

    图  9  试样爆破破碎

    Figure  9.  Fragments of specimens

    图  10  试样爆破块度分布

    Figure  10.  Specimen fragmentation size distributions

    图  11  特征块度变化

    Figure  11.  Characteristic size variation

    图  12  数值模型及网格划分

    Figure  12.  Numerical model and meshing

    图  13  钻孔周围应变场的演变

    Figure  13.  Evolution of the strain field around the borehole

    图  14  完整试样爆破块度分布实验结果与数值计算结果对比

    Figure  14.  Comparison of experimental and numerical results of fragmentations distribution on intact specimen

    图  15  有效应力分布云图

    Figure  15.  Cloud chart of effective stress distribution

    图  16  试样中有效应力的传播

    Figure  16.  Propagation of effective stress in the specimen

    图  17  应力衰减曲线

    Figure  17.  Stress attenuation

    图  18  穿节理透射

    Figure  18.  Transmission across the joint

    图  19  有效塑性应变云图

    Figure  19.  Cloud chart of effective plastic strain

    图  20  试样裂纹玫瑰图及裂纹分布

    Figure  20.  Crack rose diagram and crack distribution of samples

    图  21  圆柱形p波通过节理面传播示意图

    Figure  21.  Schematic diagram of cylindric p-wave propagation through a joint plane

    图  22  节理面上的应力分量

    Figure  22.  Stress component on the joint plane

    图  23  反射系数与h/r0的关系

    Figure  23.  Reflection coefficient vs. h/r0

    图  24  不同倾斜节理爆破能量消耗示意图

    Figure  24.  Schematic diagram of energy consumption during blasting for different inclined joints

    表  1  材料基本力学参数

    Table  1.   Basic mechanical parameters of materials

    材料类型 ρ/(kg·m−3) fc/MPa ft/MPa) E/GPa ν
    混凝土 2162 43.85 2.19 20.7 0.23
    石膏砂浆 1905 7.4 1.45 1.56 0.32
     注:ρ为密度,fc为抗压强度,ft抗拉强度,E为弹性模量,ν为泊松比.
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  • 收稿日期:  2024-10-29
  • 修回日期:  2025-04-22
  • 网络出版日期:  2024-12-10

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