Analytical method for calculating the strength limit of rock specimens of wedge form of destruction at linear distributing of contact normal tensions

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Abstract

Abstract. An analytical method for calculating the parameters of the “stress – deformation” diagrams of prismatic samples with their wedge-shaped destruction is presented based on the distribution of the L. Prandtl contact stresses with using experimental values of four indicators of rock properties: shear resistance limit, internal and external friction coefficients, elastic modulus, which can be determined experimentally by simple methods in mining enterprises, where the calculation results can be promptly used. The method is based on the theory of local destruction of rocks along sliding lines developed by the authors. The theory makes it possible to determine the current values of the normal stresses at the crack tip during its development. As a strength criterion, the Coulomb strength criterion was adopted, supplemented by the authors by taking into account contact friction. The regularities of the distribution of normal stresses from contact friction were previously established by E.P. Unksov and L. Prandtl. The regularity of E.P. Unksov was used by the authors earlier to develop a method for calculating the strength limit of rock samples of the mentioned form of destruction. In this paper, the method is based on the method of L. Prandtl. To determine the strength limit, it was necessary to develop a method for calculating the parameters of “normal stress – longitudinal deformation” diagrams. The fact is confirmed that the stress at which the crack is formed is not the limit strength. The limit strength in the case of wedge-shaped destruction of the samples is the maximum value of the normal stress on the out-of-limit branch of the “stress- deformation” diagram. Some exorbitant curves have stress discharge, which are confirmed by experimental observations. At the moment of discharge, areas appear in the form of a so-called yield tooth, the formation of which we explain by the stresses discharge on the convex part of the slip line. In the middle part, the out-of-limit curves have stress jumps, which indicate the strengthening of the samples, which have not yet received any theoretical justification. We explain this phenomenon by the transition of the destruction process from the convex part of the slip line to the concave one. Comparison of the calculated strength limit of prismatic samples obtained according to the laws of distribution of contact normal stresses, exponential – by E.P. Unksov and linear – by L. Prandtl testifies to their practical identity. Keywords:rock, strength limit, destruction, crack, “stress – deformation” diagram.
接触法向张力线性分布时楔形破坏岩样强度极限的解析计算方法
摘要基于L. Prandtl接触应力的分布,采用四种岩石性质指标的实验值,提出了一种计算楔形破坏棱柱状试样“应力-变形”图参数的解析方法:抗剪极限、内摩擦系数、外摩擦系数、弹性模量,可在矿山企业用简单的方法实验确定,计算结果可及时应用。该方法基于作者提出的沿滑动线岩石局部破坏理论。该理论使得在裂纹发展过程中确定裂纹尖端的法向应力的电流值成为可能。强度准则采用库仑强度准则,同时考虑接触摩擦。接触摩擦法向应力分布的规律是由E.P. Unksov和L. Prandtl建立的。作者早先利用E.P. Unksov的规律,开发了一种计算上述破坏形式的岩样强度极限的方法。本文的方法是基于L. Prandtl方法。为了确定强度极限,有必要开发一种计算“法向应力-纵向变形”图参数的方法。事实证明,裂纹形成时的应力不是极限强度。试样楔形破坏时的极限强度为“应力-变形”图的极限分支上的正应力最大值。一些过高曲线有应力释放,实验结果证实了这一点。在放电的时刻,区域以所谓的屈服齿的形式出现,我们用滑移线凸部的应力放电来解释其形成。在中间部分,超出极限的曲线出现了应力跳变,这表明了试样的强化,但还没有得到任何理论的证明。我们用滑移线的破坏过程从凸部过渡到凹部来解释这一现象。通过对比E.P. Unksov和L. Prandtl根据接触法向应力的指数分布规律和线性分布规律计算出的棱柱体试样的强度极限,证明了它们在实际应用中的一致性。关键词:岩石,强度极限,破坏,裂纹,“应力变形”图。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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