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首页> 外文期刊>Rock Mechanics and Rock Engineering >Numerical Investigation of Radial Strain-Controlled Uniaxial Compression Test of aspo Diorite in Grain-Based Model
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Numerical Investigation of Radial Strain-Controlled Uniaxial Compression Test of aspo Diorite in Grain-Based Model

机译:基于谷物模型的ASPO Diorite径向应变控制单轴压缩试验的数值研究

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摘要

A complete stress-strain curve is difficult to obtain for Class II rocks because of the abrupt failure after peak stress. Although the servo-controlled loading system has been used successfully in laboratory tests to analyze the failure of Class II rocks, improved simulation techniques are still needed to control the failure of Class II rocks. In this study, the Class II behavior of aspo diorite was reproduced explicitly using the GBM-UDEC model. The relative differentiations in all mechanical properties between the simulation and laboratory tests were within +/- 5%, such as Young's modulus, and slope of the post-peak stress-strain curve. Based on the stress and crack generation in UCS test simulation, the failure behavior of the aspo diorite in the post-peak stress region could be classified into three stages: (V) unstable crack growth with decreasing stress, (VI) stable crack growth with increasing stress, (VII) unstable crack growth, and failure of the rock specimen with decreasing stress. Throughout the simulation, the microcrack investigation was conducted in the aspect of number, angle, relative strength of contacts, and location. In the pre-peak stress region, the cracks between 0 degrees and 20 degrees with respect to axial stress was dominant with over 62% of population among total cracks. Cracks were generated preferentially in relatively weak contacts. The ratio of brakeage in the weakest contact was 22%, while the average breakage value of the other stronger contacts was 16%. In the post-peak stress region, the number of cracks generated between 20 degrees and 40 degrees was approximately 1.4 times higher than those between 0 degrees and 20 degrees at Stages V and VII. There was a significant increase in the number of cracks in the strongest contacts when the model was at the beginning of Stage V and Stage VII. In Stage VII, microcracks were generated intensively in central column of the rock model. Moreover, crack coalescence was monitored in the inner column and rock spalling, complete detachment of block in rock specimen model, was observed at the lateral side of the rock model in Stage VII. In the energy calculation, 23% of the strain energy stored in the model was extracted immediately after peak stress to prevent the violent failure of the rock and most of the energy extracted resulted from grain blocks compared to contacts.
机译:由于峰值应力后突然发生故障,因此难以获得完全应力 - 应变曲线。尽管在实验室测试中已成功使用伺服控制的装载系统以分析II类岩石的故障,但仍然需要改进的仿真技术来控制II级岩石的失败。在这项研究中,使用GBM-UDEC模型明确地复制了ASPO Diorite的II类行为。模拟和实验室测试之间的所有机械性能的相对分化在+/- 5%之内,例如杨氏模量和后峰值应力 - 应变曲线的斜率。基于UCS测试模拟中的应力和裂缝产生,后峰值应力区域中的ASPO Diorite的失效行为可以分为三个阶段:(v)随着应力降低的不稳定裂纹增长,(VI)稳定的裂纹生长增加压力,(vii)不稳定的裂缝生长,并且岩石标本的损失降低降低。在整个模拟中,在触点的数量,角度,相对强度和位置的相对强度方面进行微裂纹调查。在预峰值应力区域中,在0度和20度相对于轴向应力之间的裂缝是显性的,总裂缝中的超过62%的群体。优先在相对薄弱的接触中产生裂缝。 Brakeage在最弱的接触中的比例为22%,而另一个较强的接触的平均断裂值为16%。在后峰值应力区域中,在20度和40度之间产生的裂缝的数量大约在阶段V和VII之间的0度和20度之间的1.4倍。当模型处于第五阶段的开始和阶段VII的开始时,最强烈的接触中的裂缝数量显着增加。在第七阶段,在岩石模型的中央栏中产生微裂纹。此外,在内柱和岩石剥落中监测裂缝结合,在岩石模型中完全分离岩石模型,在阶段VII岩石模型的横向侧观察到。在能量计算中,在峰值应力之后立即提取储存在模型中的23%的应变能量,以防止岩石的剧烈失效,并且与触点相比,从晶粒块中提取的大部分能量产生的能量。

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