Xu Ying, Yu Yuchao, Yao Wei, Xia Kaiwen, Tang Junxi, Zhan Zhifeng
State Key Laboratory of Hydraulic Engineering Simulation and Safety, School of Civil Engineering, Tianjin University, Tianjin, 300072 China.
State Key Laboratory of Explosion Science and Technology, Beijing Institute of Technology, Beijing, 100081 China.
Geomech Geophys Geo Energy Ge Resour. 2023;9(1):17. doi: 10.1007/s40948-023-00563-x. Epub 2023 Feb 22.
A novel transient unloading testing system was adopted to simulate the transient excavation of tunnels under different lateral pressure coefficients ( ). The results show that the transient excavation of a tunnel induces significant stress redistributions and concentrations, particle displacements and vibrations to the surrounding rocks. The decrease of enhances the dynamic disturbance of transient tunnel excavation, and especially when = 0.4 and 0.2, the tensile stress can be observed on the top of the tunnel. The peak particle velocity (PPV) of the measuring points on the top of the tunnel decreases with the increasing distance between the tunnel boundary and measuring point. The transient unloading wave is generally concentrated on lower frequencies in the amplitude-frequency spectrum under the same unloading conditions, especially for lower values. In addition, the dynamic Mohr-Coulomb criterion was used to reveal the failure mechanism of a transient excavated tunnel by involving the loading rate effect. It is found that the excavation damaged zone (EDZ) of the tunnel is dominated by the shear failure, and the number of the shear failure zones increases with the decrease of . The EDZ of tunnels after transient excavations varies from ring-shape to egg-shape and X-type shear with the decrease of . The evolution of the EDZ induced by the transient unloading is associated with , i.e., the shear failure of surrounding rocks mainly occurs in the stress redistribution stage under high (1.0-0.7), while the dramatic destruction of surrounding rocks is more prone to occur after the transient unloading process when ≤ 0.6.
采用一种新型瞬态卸载试验系统来模拟不同侧压力系数( )下隧道的瞬态开挖。结果表明,隧道的瞬态开挖会引起显著的应力重新分布和集中、颗粒位移以及对周围岩石的振动。 的减小会增强瞬态隧道开挖的动态扰动,特别是当 = 0.4和0.2时,在隧道顶部可观察到拉应力。隧道顶部测量点的峰值颗粒速度(PPV)随着隧道边界与测量点之间距离的增加而减小。在相同的卸载条件下,瞬态卸载波在幅频谱中一般集中在较低频率,尤其是对于较低的 值。此外,通过考虑加载速率效应,采用动态莫尔 - 库仑准则来揭示瞬态开挖隧道的破坏机制。发现隧道的开挖损伤区(EDZ)以剪切破坏为主,并且剪切破坏区的数量随着 的减小而增加。随着 的减小,瞬态开挖后隧道的EDZ从环形变为卵形和X型剪切。瞬态卸载引起的EDZ的演化与 有关,即围岩的剪切破坏主要发生在高 (1.0 - 0.7)下的应力重新分布阶段,而当 ≤ 0.6时,围岩的剧烈破坏更易发生在瞬态卸载过程之后。