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Failure Process and Stress-Strain Curve of Plane Strain Rock Specimen with Initially Random Material Imperfections

机译:具有初始随机材料缺陷的平面应变岩石试样的破坏过程和应力-应变曲线

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The failure process of heterogeneous rock specimen with initially random material imperfections in uniaxial plane strain compression and the macroscopically mechanical response are numerically modeled by using FLAC (Fast Lagrangian Analysis of Continua). A FISH function is generated to prescribe the initial imperfections within the heterogeneous specimen by using Matlab. The imperfection is weaker than the intact rock. Beyond the failure of the imperfection, it undergoes ideal plastic behavior, while intact rock exhibits linear strain-softening behavior and then ideal plastic behavior once failure occurs. The specimen with smooth ends is loaded at a constant strain rate and is divided into 3200 elements. The maximum numbers of the initial imperfections in five schemes are 100,300, 500, 700 and 900. The effects of the number of the imperfections on the fracture process, the final fracture pattern and the complete stress-strain curve are investigated. Prior to the peak stress, some imperfections extend in the axial direction and then a part of them coalesce to form inclined shear bands. Beyond the peak stress, shear bands progressively intersect the specimen; in the process the number of the yielded elements approximately remains a constant. With an increase of the number of the initial imperfections, the spacing of shear fractures decreases, the peak stress and corresponding axial strain decrease; the post-peak branch of stress-strain curve becomes steeper; much more elements fail in tension; the number of the yielded elements in tension in the vicinity of the two lateral edges of the specimen remarkably increases.
机译:使用FLAC(快速连续拉格朗日分析),对单轴平面应变压缩中​​具有初始随机材料缺陷的非均质岩石试样的破坏过程和宏观力学响应进行了建模。通过使用Matlab,可以生成FISH函数以规定异质样本中的初始缺陷。缺陷比完整的岩石要弱。除缺陷的破坏之外,它还具有理想的塑性行为,而完整的岩石表现出线性应变软化行为,一旦发生破坏,则表现出理想的塑性行为。两端光滑的试样以恒定的应变速率加载,并分为3200个元素。五个方案中初始缺陷的最大数量为100,300、500、700和900。研究了缺陷数量对断裂过程,最终断裂模式和完整应力-应变曲线的影响。在峰值应力之前,一些缺陷会沿轴向延伸,然后它们的一部分会聚结形成倾斜的剪切带。除峰值应力外,剪切带逐渐与试样相交。在此过程中,屈服元素的数量大致保持恒定。随着初始缺陷数量的增加,剪切裂缝的间距减小,峰值应力和相应的轴向应变减小。应力-应变曲线的峰后分支变得更陡峭;更多的因素在紧张中失败;试样的两个侧边缘附近的受拉屈服元素的数量显着增加。

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