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王凯飞,张昌锁,郝兵元,等. 高地力环境下聚能爆破动、静作用对岩石内裂纹起裂与扩展机理研究[J]. 煤炭科学技术,2023,51(S1):50−64

. DOI: 10.13199/j.cnki.cst.2022-1042
引用本文:

王凯飞,张昌锁,郝兵元,等. 高地力环境下聚能爆破动、静作用对岩石内裂纹起裂与扩展机理研究[J]. 煤炭科学技术,2023,51(S1):50−64

. DOI: 10.13199/j.cnki.cst.2022-1042

WANG Kaifei,ZHANG Changsuo,HAO Bingyuan,et al. Study on initiation and propagation mechanism of internal cracks caused by dynamic and static action of shaped charge blasting under in-situ stress[J]. Coal Science and Technology,2023,51(S1):50−64

. DOI: 10.13199/j.cnki.cst.2022-1042
Citation:

WANG Kaifei,ZHANG Changsuo,HAO Bingyuan,et al. Study on initiation and propagation mechanism of internal cracks caused by dynamic and static action of shaped charge blasting under in-situ stress[J]. Coal Science and Technology,2023,51(S1):50−64

. DOI: 10.13199/j.cnki.cst.2022-1042

高地力环境下聚能爆破动、静作用对岩石内裂纹起裂与扩展机理研究

Study on initiation and propagation mechanism of internal cracks caused by dynamic and static action of shaped charge blasting under in-situ stress

  • 摘要: 深部硬岩深孔爆破弱化是一个爆炸动静荷载与地应力耦合作用下的无自由面爆破过程,地应力对爆破裂纹扩展具有很强的抑制作用,这极大地限制了深孔爆破在工作面硬岩的预弱化及切顶卸压等工程中的应用。为了探索地应力影响下的无限岩石爆破中应力波与爆生气体二者对裂纹起裂与扩展的作用机理,采用爆炸力学与断裂力学理论推导了聚能爆破动作用阶段的裂纹长度,利用LS-DYNA软件研究了地应力作用下聚能爆破动、静作用下的岩石内裂纹起裂与扩展过程。结果表明:① 数值模拟结果指向动、静作用的时间分界点为32 μs,聚能爆破动作用阶段对裂纹的起裂及初始扩展占主导地位,爆生气体静作用对裂纹的后期扩展占主导。② 无地应力作用时,静作用阶段裂纹扩展长度是应力波动作用阶段的11倍。地应力为20 MPa时,聚能爆破中动作用阶段裂纹长度被抑制了12.4%,静作用阶段裂纹长度被抑制了86.3%,地应力主要对后期爆生气体静作用阶段的裂纹扩展起抑制作用;侧向地应力垂直于裂纹扩展方向时,其抑制作用随侧向地应力增大而减弱;③ 依托古城矿N1302工作面切顶卸压工程背景,在考虑现场地应力及施工条件下,通过数值模拟最终确定最佳不耦合系数为1.3,孔间距为1 000 mm。爆后工程检验效果良好,孔内形成定向预裂缝。

     

    Abstract: Deep hard rock blasting is a free surface blasting process under the coupling effect of explosive dynamic and static load and in-situ stress. In-situ stress has a strong inhibition effect on blasting crack propagation, which greatly limits the application of deep hole blasting in the engineering of hard rock pre-weakening and roof cutting and pressure relief. In order to clarify the action mechanism of stress wave and explosive gas on crack initiation and propagation in infinite rock blasting under the influence of in-situ stress, based on explosion mechanics and fracture mechanics, the length of guided crack in shaped charge blasting action was theoretically deduced. Combined with LS-DYNA software, the process of crack initiation and propagation in rock under dynamic and static action of shaped charge blasting with or without the influence of ground stress is simulated and analyzed visually. The results show that: 1) The numerical simulation results indicate that the time cut-off point of dynamic and static action is 32 μs, and the phase of shaped charge blasting action is dominant for crack initiation and initial propagation. The static action of explosive gas is the dominant factor for crack propagation. 2) When there is no in-situ stress, the crack propagation length in the phase of static action is 11 times longer than that in the phase of stress wave action. Compared with the condition without in-situ stress, when the in-situ stress is 20 MPa, the crack length in the action stage of shaped blasting is inhibited by 12.4%, and the crack length in the static action stage is inhibited by 86.3%. The in-situ stress mainly inhibits the crack growth in the static action stage of the later explosive gas. When the lateral stress is perpendicular to the direction of crack growth, the inhibitory effect decreases with the increase of the lateral stress. 3) Based on the background of roof cutting and pressure relief engineering of N1302 working face in Gucheng Mine, the crack propagation mechanism of in-situ stress and dynamic and static action of deep-hole blasting was considered through numerical simulation, and the optimal decoupling coefficient was finally determined to be 1.3, and the hole spacing was1000mm. The engineering inspection effect after explosion was good, and directional pre-cracks were formed in the hole.

     

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