Fracturing responses, mechanical behaviors and anchoring effects for rough layered rock mass

IF 2.8 3区 工程技术 Q1 MATHEMATICS, INTERDISCIPLINARY APPLICATIONS Computational Particle Mechanics Pub Date : 2024-03-02 DOI:10.1007/s40571-024-00726-x
Yajun Ren, Qian Yin, Zhigang Tao, Jiangyu Wu, Yaoyao Meng, Hongwen Jing, Lulin Zheng, Hai Pu, Junjie Li, Qingxiang Meng
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Abstract

This study is based on indoor experiments using PFC2D to conduct numerical tests on the uniaxial compression of layered rock masses with multiple sets of parallel rough joints at a loading rate of 0.1 m/s. The layered rock mass is composed of hard matrix and weak interlayer, with uniaxial compressive strengths of 45.43 MPa and 16.08 MPa and elastic moduli of 4.47 GPa and 3.20 GPa, respectively. This study numerically investigated the influences of bedding inclination α (0°–90°), joint roughness coefficient JRC (0–19.55) and anchor bolts on crack propagation, fracturing responses, crack initiation stress, mechanical properties, ultimate failure modes, and brittleness index for the rough layered rock mass. The results show that, with an increasing bedding inclination, the peak strength of the layered samples exhibits a “U”-shaped variation trend, first decreasing and then increasing. For the bedding inclination = 30°–75°, the peak strength increases with an increasing JRC. The failure modes of the sample are mainly influenced by the bedding inclination. For the bedding inclination = 0°–30° and 90°, the samples mainly experience tensile splitting failure. For the bedding inclination = 45°–75°, the samples undergo shear slip failure along the weak interlayer. The crack initiation stress of the layered samples first decreases and then increases with an increasing bedding inclination and increases with an increasing JRC. The peak strength and failure mode of the samples are both functions of the bedding inclination and JRC. Based on the different failure modes, a nonlinear strength failure criterion for the layered rock masses with multiple sets of parallel rough joints is established. Comparison with the experimental results shows that this criterion can better reflect the mechanical properties of layered rock masses. Anchor bolts can effectively increase the peak strength, reduce the brittleness characteristics, and restrict the shear slip deformation for the samples. The peak strength increases by 18.03–26.21% with an increasing initial anchoring force (0–20 MPa). When the anchoring force is 10 MPa, the peak strength of the anchored samples decreases first and then increases regarding the bedding inclination. Compared with the unanchored samples, the peak strength increases by 9.44–42.13% and the brittleness index decreases by 18.58–72.44%. The peak strength of the anchored samples increases with JRC. Compared with unanchored samples, the peak strength increases by 14.72–26.21%, while the brittleness index decreases by 69.05–73.19%.

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粗糙层状岩体的断裂响应、力学行为和锚固效应
本研究基于室内实验,使用 PFC2D 对具有多组平行粗糙节理的层状岩体在 0.1 m/s 加载速率下的单轴压缩进行了数值试验。层状岩体由硬基体和弱夹层组成,单轴抗压强度分别为 45.43 MPa 和 16.08 MPa,弹性模量分别为 4.47 GPa 和 3.20 GPa。本研究通过数值方法研究了垫层倾角α(0°-90°)、节理粗糙度系数JRC(0-19.55)和锚杆对粗糙层状岩体的裂纹扩展、断裂响应、裂纹起始应力、力学性能、极限破坏模式和脆性指数的影响。结果表明,随着垫层倾角的增大,层状岩样的峰值强度呈 "U "形变化趋势,先减小后增大。在垫层倾角 = 30°-75° 时,峰值强度随 JRC 的增大而增大。试样的破坏模式主要受垫层倾角的影响。在垫层倾角 = 0°-30° 和 90° 时,样品主要经历拉伸劈裂破坏。在垫层倾角=45°-75°时,试样沿薄弱夹层发生剪切滑移破坏。分层试样的裂纹起始应力随着垫层倾角的增大先减小后增大,并随着 JRC 的增大而增大。样品的峰值强度和破坏模式都是垫层倾角和 JRC 的函数。根据不同的破坏模式,建立了具有多组平行粗糙节理的层状岩体的非线性强度破坏准则。与实验结果比较表明,该准则能更好地反映层状岩体的力学特性。锚杆能有效提高样品的峰值强度,降低脆性特征,限制剪切滑移变形。随着初始锚固力(0-20 兆帕)的增加,峰值强度增加了 18.03%-26.21%。当锚固力为 10 兆帕时,锚固样品的峰值强度先降低,然后随着垫层倾斜度的增加而增加。与未锚固样品相比,峰值强度增加了 9.44-42.13%,脆性指数降低了 18.58-72.44%。锚固样品的峰值强度随 JRC 的增加而增加。与未锚固样品相比,峰值强度增加了 14.72-26.21%,而脆性指数降低了 69.05-73.19%。
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来源期刊
Computational Particle Mechanics
Computational Particle Mechanics Mathematics-Computational Mathematics
CiteScore
5.70
自引率
9.10%
发文量
75
期刊介绍: GENERAL OBJECTIVES: Computational Particle Mechanics (CPM) is a quarterly journal with the goal of publishing full-length original articles addressing the modeling and simulation of systems involving particles and particle methods. The goal is to enhance communication among researchers in the applied sciences who use "particles'''' in one form or another in their research. SPECIFIC OBJECTIVES: Particle-based materials and numerical methods have become wide-spread in the natural and applied sciences, engineering, biology. The term "particle methods/mechanics'''' has now come to imply several different things to researchers in the 21st century, including: (a) Particles as a physical unit in granular media, particulate flows, plasmas, swarms, etc., (b) Particles representing material phases in continua at the meso-, micro-and nano-scale and (c) Particles as a discretization unit in continua and discontinua in numerical methods such as Discrete Element Methods (DEM), Particle Finite Element Methods (PFEM), Molecular Dynamics (MD), and Smoothed Particle Hydrodynamics (SPH), to name a few.
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