关于剪切驱动干扰中放松时间的考虑
Lucas Hedström1, Peter Olsson1
1Department of Physics, <a href="https://ror.org/05kb8h459">Umeå University</a>, 901 87 Umeå, Sweden.
Physical review. E
|July 18, 2024
概括
我们研究了在剪切下弹性粒子的干扰过渡,专注于放松时间. 压力相关性被发现比放松时间相关性寿命更长,影响了关键指数的确定.
科学领域:
- 物理 物理学 物理
- 材料科学 材料科学 材料科学
- 统计力学 统计力学
背景情况:
- 干扰过渡是各种混乱系统中观察到的关键现象.
- 了解堵塞点附近的动态对于预测材料特性至关重要.
研究的目的:
- 为了研究在零温度下剪切下的弹性粒子模型中的干扰过渡.
- 在干扰过渡期间分析放松时间 (τ1) 和与压力 (p1) 的相关性.
主要方法:
- 两步模拟:初始剪切,然后进行能量放松.
- 从指数式能量衰变中确定放松时间 (τ1).
- 分析 τ1,压力 (p1) 和剪切变量 (γ) 之间的相关性.
主要成果:
- 发现压力相关性 (p1) 的寿命比放松时间相关性 (τ1) 的寿命更长.
- 个体t1受到起始配置的压力 (p1) 和随机贡献的影响,这取决于放松路径的长度.
- 一个特定的剪切变量,由t1相关性得出的gτ,被确定为关键指数的确定.
结论:
- 压力和放松动态之间的相互作用决定了干扰过渡.
- 已识别的 γτ 提供了一个更准确的参数,用于在剪切颗粒系统中表征关键指数.
- 这项研究提供了关于点附近无序材料复杂行为的见解.
相关概念视频
Atomic Nuclei: Types of Nuclear Relaxation
284
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
284
Shearing Stress
541
Shearing stress, denoted by the Greek letter tau (τ), is stress caused by forces acting transversely on an object. These forces create internal ones within the entity in the plane where the external forces are applied. The resultant of these internal forces is the shear in the section.
The average shearing stress can be calculated by dividing the shear by the area of the cross-section.
The average shearing stress can be calculated by dividing the shear by the area of the cross-section.
541
Elastic Strain Energy for Shearing Stresses
182
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...
182
Shearing Strain
252
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...
252
Problem Solving on Stress and Strain
725
Stress is a quantity that describes the magnitude of a force that causes deformation, generally defined as internal force per unit area. When forces pull on an object and cause its elongation, like the stretching of an elastic band, it is called tensile stress. When forces cause the compression of an object, it is known as compressive stress. When an object is being squeezed uniformly from all sides, like a submarine in the depths of the ocean, we call this kind of stress bulk stress (or volume...
725
Atomic Nuclei: Nuclear Relaxation Processes
644
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
644


