围压作用下Inada花岗岩强度分布及蠕变破坏时间

T. Yamaguchi, S. Okub, E. Maranini
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引用次数: 1

摘要

在设计岩体深部地下结构的长期稳定性时,需要估算围压作用下岩石的蠕变破坏时间。以核废料处置隧道为例,蠕变破坏时间应超过1万年。本文介绍了三轴蠕变和多级蠕变试验的实验结果。两种试验均在围压高达40 MPa、单轴应力状态下进行。为了消除分析中强度对加载速率的依赖,引入了标准化强度的概念。应用Janach破坏准则成功地解释了标准强度与围压之间的关系。我们引入了归一化破坏时间的新概念,该概念被认为是确定特定岩石试件强度和/或蠕变破坏时间的最重要的价值。结果表明,由实验结果估计的归一化失效次数的色散近似为威布尔分布。给出了归一化破坏时间与强度和/或蠕变破坏时间的换算公式。利用该换算公式,在40mpa围压下,为保证99%的试件10000年后的存续率,蠕变应力水平应小于79%。通过归一化破坏时间,不仅可以计算出蠕变破坏次数的分布,还可以计算出任意加载速率和围压下的强度分布。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Distributions of strength and creep failure time of Inada granite under confining pressure
In designing the long-term stability of deep underground structures in a rock mass, it is necessary to estimate the creep failure time of rocks under confining pressure. In the case of nuclear waste disposal tunnel, the creep failure time should exceed 10,000 years. In this paper, experimental results of tri-axial and multi-stage creep experiments are presented. Both kinds of experiments were conducted under confining pressures up to 40 MPa, includ-ing uni-axial stress state. In order to eliminate the loading rate dependency of strength in analysis, the concept of standardized strength is introduced. The Janach's failure criterion was successfully applied to explain the relation between standardized strengths and confining pressures. We introduce a new concept of normalized failure time that is thought to be most substantial value in determining the strength and / or creep failure time of a specific rock specimen. It is shown that the dispersion of normalized failure times, which was estimated from the experimental results, exhibited approximately a Weibull distribution. A conversion formula from normalized failure time to strength and / or creep failure time is presented. Using this conversion formula, we showed that creep stress level should be less than 79 % for survival of 99 % of test pieces after 10,000 years under the confining pressure of 40 MPa. It is also shown that not only the distribution of creep failure times, but also the strength distribution under any loading rate and confining pressure can be calculated from the normalized failure time.
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