在方向剪切应力路径下,类似弱固软岩的非同轴可塑性
Jiashun Liu1,2,3, Zhiyong Zheng4, Hui Zhou5
1School of Civil Engineering, Liaoning Technical University, Fuxin, 123000, People's Republic of China. liujiashun000@163.com.
Scientific reports
|September 10, 2024
概括
这项研究揭示了软岩在复杂应力下表现出非同轴塑料流,这是传统理论未能捕捉到的现象. 开发并验证了软岩力学中非同轴特征的新量化方法.
科学领域:
- 地质技术工程 地质技术工程
- 岩石机械学 岩石机械学
- 连续力学 连续力学
背景情况:
- 在复杂的应力路径下,软岩塑料流显示非同轴特征.
- 传统的可塑性理论不能充分反映这些行为,使软岩的失败机制不清楚.
研究的目的:
- 在软岩石中研究微弱凝固的应变增量和非同轴特征的演变.
- 开发和验证一种新的方法来量化软岩中的非同轴性行为.
主要方法:
- 使用空心筒装置 (HCA) 进行方向剪切测试.
- 应力速率的分解成大小和方向.
- 对于塑料流动方向的球形插曲系数方法.
- 引入一个非同轴参数 (Δ).
主要成果:
- 当α角为0°或90°时,非同轴性是不存在的.
- 非同轴角度振荡在张力扭转中比压力扭转更为明显.
- 当样本接近失败时,非同轴性会消散.
- 拟议的方法有效地捕捉了主要应力方向对非同轴行为的影响.
结论:
- 开发的方法准确量化了软岩石中的非同轴特性.
- 这项研究为了解软岩力学和故障机制提供了重大进展.
相关概念视频
Plastic Behavior
192
A material's elastic behavior is characterized by the disappearance of stress once the load is removed, allowing the material to return to its original state. However, when stress surpasses the yield point, yielding commences, marking the onset of plastic deformation or permanent set. This change from elastic to plastic behavior is influenced by the peak stress value and the duration before the load is removed. An intriguing observation occurs when a specimen is loaded, unloaded, and...
192
Relation between Poisson's ratio, Modulus of Elasticity and Modulus of Rigidity
253
Deformation occurs in axial and transverse directions when an axial load is applied to a slender bar. This deformation impacts the cubic element within the bar, transforming it into either a rectangular parallelepiped or a rhombus, contingent on its orientation. This transformation process induces shearing strain. Axial loading elicits both shearing and normal strains. Applying an axial load instigates equal normal and shearing stresses on elements oriented at a 45° angle to the load axis.
253
Plastic Deformations
84
It is essential to understand how structural members behave under plastic deformation when the bending stress exceeds the material's yield strength. This state of deformation permanently alters the shape of the member, in contrast to the linear elastic behavior observed before yielding. The strain at any point in the member is expressed in terms of maximum strain. Notably, the neutral axis, which coincides with the centroid during elastic bending, shifts away from the centroid under plastic...
84
Elastic Strain Energy for Shearing Stresses
171
As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
171
Shearing Strain
235
The shearing strain represents a cubic element's angular change when subjected to shearing stress. This type of stress can transform a cube into an oblique parallelepiped without influencing normal strains. The cubic element experiences a significant transformation when exposed solely to shearing stress. Its shape alters from a perfect cube into a rhomboid, clearly demonstrating the effect of shearing strain. The degree of this strain is considered positive if it reduces the angle between...
235
Plastic Deformations of Members with a Single Plane of Symmetry
86
When a structural member undergoes plastic deformation due to bending, it is crucial to understand the position of the neutral axis and the stress distribution. This member, characterized by a single plane of symmetry, exhibits a uniform stress distribution, with negative stress above the neutral axis and positive stress below. Notably, the neutral axis does not align with the centroid of the cross-section. This misalignment is typical in cases where the cross-section is not rectangular or...
86


