Simulation of Meso-mechanism of Lac du Bonnet Granite Failure Based on Elasto-plastic PFC3D Constitutive Model

PENG Shu-quan, LIU Qin, BAO Zhuo-ran, FAN Ling

Journal of Changjiang River Scientific Research Institute ›› 2020, Vol. 37 ›› Issue (1) : 142-148.

PDF(2593 KB)
PDF(2593 KB)
Journal of Changjiang River Scientific Research Institute ›› 2020, Vol. 37 ›› Issue (1) : 142-148. DOI: 10.11988/ckyyb.20180319
ROCKSOIL ENGINEERING

Simulation of Meso-mechanism of Lac du Bonnet Granite Failure Based on Elasto-plastic PFC3D Constitutive Model

  • PENG Shu-quan, LIU Qin, BAO Zhuo-ran, FAN Ling
Author information +
History +

Abstract

A novel constitutive model was presented in line with the ideal elasto-plastic rolling and twisting moment and the Mohr-Coulomb-maximum-tensile failure criterion. The model could reflect four failure modes: tensile failure, compression-shear failure, rolling yielding, and twisting yielding. The model was incorporated into PFC3D with secondary development to set up the equations of macro-and-mesoscopic parameters and to simulate the mesoscopic failure mechanism of Lac du Bonnet (LDB) granite in compression-shear test and tensile test. According to the results, the significant effects of particle rolling and twisting on the macro-cohesion and frictional angle of rock were observed. The macro-cohesion also increased to a constant value with the growth of mesoscopic ultimate moment and torque and meso-cohesion. The macroscopic internal friction angle increased with the increasing of mesoscopic ultimate moment and torque and mesoscopic frictional coefficient. The macroscopic tensile strength increased with the increase of microscopic tensile stress until reaching a constant value. The macroscopic elastic modulus and the Poisson’s ratio were mainly determined by mesoscopic elastic modulus of particles and their stiffness ratio. The numerical simulation result of LDB granite by the presented model was well consistent with indoor experimental results in terms of strength and deformation behaviors, compressive strength to tensile strength ratio as well as crack distribution. Before reaching to the peak value, the mesoscopic tensile cracks were dominant cracks in the LDB granite extending in an “X” shape from the end of specimen towards the middle of specimen under the condition of vertical-low pressure. Under the conditions of vertical pressure close to the peak value or exceeding the peak value, meso-cracks of compression-shear, and meso-failure of rolling and twisting were found. The cracks developed from the bottom to the top of specimen, with dip angles equal to the macro failure angle of LDB granite. And that reveals the mesoscopic mechanism of macro-cracks of LDB granite.

Key words

Lac du Bonnet granite / ideal elasto-plastic rolling-twisting model / Mohr-Coulomb maximum-tensile criterion / discrete element / 3D particle flow / macroscopic and mesoscopic parameters / cracks

Cite this article

Download Citations
PENG Shu-quan, LIU Qin, BAO Zhuo-ran, FAN Ling. Simulation of Meso-mechanism of Lac du Bonnet Granite Failure Based on Elasto-plastic PFC3D Constitutive Model[J]. Journal of Changjiang River Scientific Research Institute. 2020, 37(1): 142-148 https://doi.org/10.11988/ckyyb.20180319

References

[1] WANG Y, TONON F. Modeling Lac du Bonnet Granite Using a Discrete Element Model[J]. International Journal of Rock Mechanics & Mining Sciences, 2009, 46(7): 1124-1135.
[2] CHO N, MARTIN C D, SEGO D C. A Clumped Particle Model for Rock[J]. International Journal of Rock Mechanics & Mining Sciences, 2007, 44(7): 997-1010.
[3] POTYONDY D O. Simulating Stress Corrosion with a Bonded-particle Model for Rock[J]. International Journal of Rock Mechanics & Mining Sciences, 2007, 44(5): 677-691.
[4] CUNDALL P A. A Computer Model for Simulating Progressive Large-Scale Movements in Block Rock Systems[C]//Proceeding of Symposium of International Society of Rock Mechanics. Rotterdam: Balkama A. A, 1971: 128-132.
[5] CUNDALL P A, STRACK O D L. A Discrete Numerical Model for Granular Assemblies[J]. Géotechnique, 1979, 29(1): 47-65.
[6] POTYONDY D O, CUNDALL P A. A Bonded-particle Model for Rock[J]. International Journal of Rock Mechanics & Mining Sciences, 2004, 41(8): 1329-1364.
[7] 赵国彦,戴 兵,马 驰. 平行黏结模型中细观参数对宏观特性影响研究[J]. 岩石力学与工程学报, 2012, 31(7): 1491-1498.
[8] 徐小敏,凌道盛,陈云敏,等. 基于线性接触模型的颗粒材料细–宏观弹性常数相关关系研究[J]. 岩土工程学报, 2010,32(7): 991-998.
[9] IWASHITA K, ODA M. Micro-deformation Mechanism of Shear Banding Process Based on Modified Distinct Element Method[J]. Powder Technology, 2000, 109(1/2/3): 192-205.
[10]KUHN M R, BAGI K. Alternative Definition of Particle Rolling in a Granular Assembly[J]. Journal of Engineering Mechanics, 2004, 130(7): 826-835.
[11]WILSON R, DINI D, WACHEM B V. The Influence of Surface Roughness and Adhesion Particle Rolling[J]. Powder Technology, 2017, 312:321-333.
[12]IWASHITA K, ODA M. Rolling Resistance at Contacts in Simulation of Shear Band Development by DEM[J]. Journal of Engineering Mechanics, 1998, 124(3): 285-292.
[13]蒋明镜, 陈 贺, 刘 芳. 岩石微观胶结模型及离散元数值仿真方法初探[J]. 岩石力学与工程学报, 2013, 32(1):15-23.
[14]蒋明镜,方 威,司马军. 模拟岩石的平行粘结模型微观参数标定[J]. 山东大学学报(工学版), 2015, 45(4): 50-56.
[15]JIANG M J, YU H S, HARRIS D. A Novel Discrete Model for Granular Material Incorporating Rolling Resistance[J]. Computers & Geotechnics, 2005, 32(5): 340-357.
[16]JIANG M J, SHEN Z F, WANG J F. A Novel Three-dimensional Contact Model for Granulates Incorporating Rolling and Twisting Resistances[J]. Computers and Geotechnics, 2015, 65: 147-163.
[17]彭述权. PFC3D-FDM多场耦合分析软件V1.0(2015SR187094) [DB/CD]. 2015.
[18]MARTIN C D. The Strength of Massive Lac du Bonnet Granite around Underground Openings[D].Manitoba: University of Manitoba, 1993.
[19]LIM S S, MARTIN C D. Core Disking and Its Relationship with Stress Magnitude for Lac du Bonnet Granite[J]. International Journal of Rock Mechanics & Mining Sciences, 2010, 47(2): 254-264.
PDF(2593 KB)

Accesses

Citation

Detail

Sections
Recommended

/