动态真三轴同步冲击下煤样变形与致灾力学机理

Dynamic deformation and disaster mechanical mechanism of coal under dynamic true triaxial synchronous impact loading

  • 摘要: 矿山地下空间再利用过程中,煤体受岩层瞬时破断、爆破和地震等多源扰动影响,处于多轴多向动力扰动作用状态,极易诱发动力灾害。深入了解煤体在三维动态应力环境中的力学响应规律对矿山地下空间安全高效再利用具有重要意义。为此,采用动态真三轴电磁霍普金森杆试验测试系统,通过调控充电电压实现煤样在10~100 s−1应变率的动态真三轴同步冲击试验,探明动态真三轴冲击作用下煤样的变形规律与致灾力学机理。试验中三轴六向应力波到达试样端面的误差在5 μs以内,幅值偏差在1%以内,实现了三轴六向应力波一致性加载;煤样各轴向平均在90 μs达到动态应力平衡状态,持续时间占比大于70%,满足了动态应力平衡要求。结果表明:随着应变率的增加,煤样峰值动态应力和应变近似线性增大,其表面裂纹逐渐增多,且在边角发生破坏,呈现显著的应变率效应,而弹性模量对应变率的变化不敏感。此外,煤样各轴向动态应力−应变曲线的峰后曲线形态均呈现应力回弹特征,表明冲击加载过程中存储的弹性能释放,导致其弹性变形恢复。随着应变率增加,煤样各轴向宏观压缩变形量逐渐减小,并在高应变率下呈现膨胀变形特征,表明压密裂纹在外部动态约束解除后重新张开。动态真三轴等幅值同步冲击作用使煤样处于近似相等的三轴动态压缩应力环境,抑制裂纹的发育及扩展,使其主体结构未发生明显宏观破坏;在动态真三轴差幅值同步冲击下,中间主应力的变化促使煤样沿最小主应力方向产生张拉变形,诱导裂纹产生剪切滑移与贯通破坏。相较于等幅值冲击作用,差幅值加载形成的主应力差更容易促使裂纹发生剪切滑移,是诱导煤体在真三轴冲击荷载下发生灾变的重要力学条件。因此,矿山地下空间再利用过程中,应重点关注多维扰动形成的三维动态主应力差,调控局部偏应力集中现象,进而降低复杂动力扰动作用下煤体发生动力灾害的风险。

     

    Abstract: During the reuse of underground space in mine, coal masses are subjected to multi-axial and multi-directional dynamic disturbances induced by multiple sources, such as instantaneous strata fracturing, blasting, and earthquakes, thereby increasing the likelihood of dynamic disasters. A comprehensive understanding of the mechanical response of coal under dynamic three-dimensional impact loading is critical for the safe and efficient reuse of underground spaces. A dynamic true triaxial electromagnetic Hopkinson bar system was employed to conduct synchronous dynamic true triaxial impact tests on coal specimens at strain rates of 10−100 s−1 by adjusting the charging voltage, elucidating their deformation behaviors and disaster-inducing mechanisms. During impact loading, the discrepancies in arrival time and amplitude of the stress waves under triaxial and six-directional synchronous loading were maintained within 5 μs and 1%, respectively, demonstrating excellent loading consistency. The specimens reached dynamic stress equilibrium along each axis at approximately 90 μs, which was maintained for more than 70% of the impact duration, thereby satisfying the requirements for dynamic stress equilibrium. The results indicate that, as the strain rate increased, the peak dynamic stress and strain of the coal specimens increased approximately linearly. Furthermore, more cracks were observed on the specimen surfaces, and local corner failure became more evident at higher strain rates. By contrast, the elastic modulus was insensitive to the strain rate; The post-peak shape of the dynamic strain stress curves along the three principal axes exhibits a stress rebound characteristic, suggesting that the stored elastic energy in the specimen during impact loading was released, leading to partial deformation recovery. As the strain rate increased, the macroscopic compressive deformation of the coal specimens in each axial direction after impact gradually decreased and even changed to expansive deformation at high strain rates, indicating the reopening of compacted cracks after external dynamic constraints were removed. Under dynamic true triaxial synchronous impact loading with equal amplitudes, the coal specimens were subjected to an approximately balanced triaxial dynamic compressive stress environment, which suppressed crack development and propagation; consequently, no significant failure occurred within the main structure. In contrast, under dynamic true triaxial synchronous impact loading with unequal amplitudes, the changes in the intermediate principal stress promoted tensile deformation of the coal specimens along the minimum principal stress direction, thereby inducing crack shear slip and through-going failure. Compared with equal-amplitude loading, unequal-amplitude loading generated a principal stress difference that more readily promoted conditions for crack shear slip. This demonstrates that the dynamic principal stress difference state is an important mechanical factor that induces dynamic disasters. Therefore, during the reuse of underground mine spaces, particular attention should be paid to variations in three-dimensional dynamic principal stress differences caused by multidirectional disturbances, and local deviatoric stress concentration should be controlled to reduce the risk of dynamic disasters in coal masses subjected to complex dynamic disturbances.

     

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