在火山岩中切换故障后变形模式.
Jamie I Farquharson1,2, Michael J Heap3,4, Lucille Carbillet5
1Institute for Research Administration, Niigata University, Ikarashi 2-8050, Nishi-ku, Niigata 950-2181, Japan.
Royal Society open science
|August 29, 2024
概括
多孔岩石在失效后可以在压缩和膨胀之间切换. 这些转变显著影响地系统中的流体流动和热传递.
科学领域:
- 地质物理学 地质物理学
- 岩石力学 岩石力学 岩石力学
- 材料科学 是一种材料科学.
背景情况:
- 多孔岩石表现出扩张或紧的不弹性变形,超过了值压力.
- 了解物理性质对变形的反应对于地质量和热传输以及压力演变至关重要.
- 观察到扩张和紧缩 (故障模式) 之间的过渡,但研究不足.
研究的目的:
- 为了研究多孔岩石中复杂的故障后变形行为.
- 阐明驱动压缩和扩张之间的过渡的机制.
- 了解这些转变对岩石物理性质的影响.
主要方法:
- 在多孔石上进行了有针对性的机械变形实验.
- 研究了一组样本和有效压力范围,跨越了压缩的正负体积反应.
- 在变形后分析物理性质的变化,特别是透性.
主要成果:
- 确定了两个故障后的关键应激状态:压缩-扩张和扩张-压缩过渡.
- 证明在浅层地条件下可以发生多个变形模式开关.
- 观察到,尽管体积变化很小,但在经历扩张到紧缩性失效的样品中,透率增加了两级.
结论:
- 在浅层地环境中,故障后变形模式的切换是显著的.
- 将扩展剂切换为紧缩剂的故障模式大大提高了透性,影响了溶液和热传递.
- 这些现象对于理解火山环境中的流体压力演变至关重要.
相关概念视频
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
Temperature Dependent Deformation
143
In a nonhomogeneous rod made up of steel and brass, restrained at both ends and subjected to a temperature change, several steps are involved in calculating the stress and compressive load. Due to the problem's static indeterminacy, one end support is disconnected, allowing the rod to experience the temperature change freely. Next, an unknown force is applied at the free end, triggering deformations in the rod's steel and brass portions. These deformations are then calculated and added...
143
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
Stress-Strain Diagram - Ductile Materials
652
The stress-strain relationship in ductile materials such as structural steel or aluminium is intricate and progresses through several stages. When a specimen is loaded, it initially exhibits a linear length increase, depicted by a steep straight line on the stress-strain diagram. It indicates the material is elastically deforming and will return to its original shape once unloaded. However, when a critical stress value is reached, plastic deformation begins. This stage sees substantial...
652
Deformation of Member under Multiple Loadings
159
When a rod is made of different materials or has various cross-sections, it must be divided into parts that meet the necessary conditions for determining the deformation. These parts are each characterized by their internal force, cross-sectional area, length, and modulus of elasticity. These parameters are then used to compute the deformation of the entire rod.
In the case of a member with a variable cross-section, the strain is not constant but depends on the position. The deformation of an...
In the case of a member with a variable cross-section, the strain is not constant but depends on the position. The deformation of an...
159
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


