STATISTICAL NATURE OF STRENGTH AND SCALE EFFECT IN MOUNTAIN ROCKS

Rafail Mehdiev Rafail Mehdiev, Gulshad Agayeva Gulshad Agayeva
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Abstract

The theories and concepts of strength considered above are based on the model of a body either as a homogeneous structureless medium, or as a material having a structure, but uniform throughout its volume. Rocks are obviously not such bodies. They are composed of mineral grains of different properties, contain macrodefects in the form of pores and various inclusions, as well as objects of various aggregate states (gases, liquids). Under these conditions, deterministic theories of strength turn out to be clearly untenable. In particular, the use of the classical theory of Griffith cracks is complicated by the following circumstance. Since the rock is an aggregate of mineral grains, a microcrack developing inside the grain inevitably reaches its boundary and, consequently, the radius r of the crack mouth increases abruptly. Therefore, for the transition of a crack to another grain and its further development, a stress greater than that follows from Griffith's theory is required. Thus, there is some "barrier" stress, at which only the development of a crack in a real rock is possible. In addition, the development of cracks in the rock occurs mainly along the contact of mineral grains, i.e., along the cementing material, often of a clay composition. For such a material, the theory of brittle fracture is applicable. The destruction of the rock (from the standpoint of any theory of strength) is determined by the stresses acting in it. But due to the heterogeneous structure of the rocks, the local stress concentration centers are randomly distributed in its volume. Therefore, the strength and destruction of rocks must be considered from a statistical standpoint. This approach is justified for most other materials used by humans. The idea of the statistical nature of strength was first put forward in scientific terms by A.P. Aleksandrov and N.S. Zhurkov in 1933. Keywords: rock strength, constant material, scale effect, rocks, destruction probability, fractured, robustness theory, microcrack, mineral, experience constant, density of defects, displacement, compression.
山岩强度和尺度效应的统计性质
上述关于强度的理论和概念都是基于这样的模型:物体要么是均匀的无结构介质,要么是有结构的材料,但在整个体积中都是均匀的。岩石显然不是这样的物体。它们由不同性质的矿物颗粒组成,含有孔隙和各种包裹体形式的宏观缺陷,以及各种聚集状态(气体、液体)的物体。在这些条件下,强度的确定性理论显然是站不住脚的。特别是,经典格里菲斯裂纹理论的应用由于以下情况而变得复杂。由于岩石是矿物颗粒的集合体,在颗粒内部发育的微裂纹不可避免地到达其边界,因此裂纹口半径r突然增大。因此,裂纹向另一晶粒的转变及其进一步发展,需要一个大于格里菲斯理论的应力。因此,存在某种“屏障”应力,在这种应力下,真正的岩石中才可能出现裂缝。此外,岩石中裂缝的发育主要沿着矿物颗粒的接触发生,即沿着胶结材料,通常是粘土成分。对于这种材料,脆性断裂理论是适用的。岩石的破坏(从任何强度理论的观点来看)是由作用在其中的应力决定的。但由于岩石的非均质结构,局部应力集中中心在其体积中是随机分布的。因此,必须从统计的角度来考虑岩石的强度和破坏。这种方法适用于人类使用的大多数其他材料。1933年,A.P. Aleksandrov和N.S. Zhurkov首次以科学术语提出了力量的统计性质。关键词:岩石强度,恒定材料,尺度效应,岩石,破坏概率,断裂,鲁棒性理论,微裂纹,矿物,经验常数,缺陷密度,位移,压缩。
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