Dynamic influence of frequent dynamic disturbance on high-energy rock mass during confining pressure unloading
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摘要: 基于冬瓜山铜矿深部巷道围岩开挖过程中面临的高应力和频繁爆破扰动问题,利用改进的SHPB动静组合加载系统,开展了频繁动力扰动对围压卸载中高储能岩体动力学影响的研究。研究结果表明,围压卸载中的矽卡岩受到动力扰动时,其动态峰值应力和弹性模量随动力扰动次数非线性变化。围压卸载中的高储能矽卡岩受到动力扰动时会释放能量。轴压促使岩样内微裂隙轴向发育,造成岩样抵抗动力扰动能力减弱;围压减缓岩样内微裂隙轴向发育,造成岩样抵抗动力扰动能力增强。动力扰动对微裂隙扩展有促进作用,使围压卸载中的岩样由拉伸破坏向剪切破坏转变。Abstract: In this study, based on the high stress and frequent blast disturbance in the process of surrounding rock excavation in the deep roadway of Dongguashan Copper Mine, we investigated the dynamic properties of the high-energy rock mass disturbed by frequent dynamic loading during confining pressure unloading, using the modified SHPB coupled static-dynamic loading system. The results show that the peak dynamic stress and elastic modulus of the skarn subjected to confining pressure unloading varied nonlinearly with the number of dynamic disturbances, and the high energy skarn in confining pressure unloading released energy when subjected to dynamic disturbance. The axial pressure promoted the axial development of micro-fissures in the rock specimens, resulting in a lower capacity of rock samples. However, the confining pressure restrained the axial development of micro-fissures in the rock sample, resulting in a higher capacity of rock samples. The dynamic disturbance promoted the micro-fracture expansion, transforming the rock sample in confining pressure from tensile failure to shear failure.
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表 1 实验方案
Table 1. Experimental plan
岩样 预加轴压
/MPa预加围压
/MPa冲击时围压
/MPa围压卸载速率
/(MPa·s−1)冲击气压
/MPaXK1-1 62.5 15 7.5 1 0.6 XK1-2 20 10 XK2-1 72.5 15 7.5 1 0.6 XK2-2 20 10 XK3-1 82.5 15 7.5 1 0.6 XK3-2 20 10 表 2 矽卡岩三轴压缩实验结果
Table 2. Triaxial compression experimental results for skarn
围压
/MPa弹性模量
/GPa三轴抗压强度
/MPa峰值应变
/10−3黏结力
/MPa内摩擦角
/(°)15 26.81 217.93 10.27 6.86 57 20 32.69 237.87 12.29 表 3 冲击次数统计表
Table 3. Summary of impacts
岩样 预加轴压/
MPa预加围压/
MPa冲击时围压/
MPa冲击次数 XK1-1 62.5 15 7.5 35 XK1-2 20 10 36 XK2-1 72.5 15 7.5 21 XK2-2 20 10 31 XK3-1 82.5 15 7.5 13 XK3-2 20 10 21 -
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