移动性诱导相位分离的格子模型中的界面和密度波动
Liheng Yao1, Robert L Jack1,2
1DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom.
The Journal of chemical physics
|March 17, 2025
概括
自行粒子表现出运动性诱导的相分离. 密度相的界面波动是由毛细血管波理论描述的,即使有内部气泡,由于时间尺度的分离.
科学领域:
- 统计力学 统计力学
- 软物质物理学 软物质物理学
- 非平衡系统 非平衡系统
背景情况:
- 机动性诱导的相分离 (MIPS) 是活性物质系统中的一个关键现象.
- 了解相隔动态和界面特性之间的相互作用至关重要.
研究的目的:
- 分析自行运动粒子的2D晶格模型中的运动诱导和泡相分离.
- 为了比较密集相的板块和滴滴几何形状.
- 为了研究界面波动和密度概况.
主要方法:
- 自动运动粒子的格子模型模拟.
- 使用毛细血管波浪理论分析界面波动.
- 液体和蒸汽密度和波动的表征.
主要成果:
- 板块几何的界面波动被毛细血管波浪理论很好地描述,尽管内部存在泡.
- 时间尺度的分离解释了毛细管波理论的适用性.
- 蒸汽相表现出与拉普拉斯压力效应和高斯波动的平衡状行为.
- 液相表现出很大的非高斯波动,没有显著的密度转移.
结论:
- 毛细管波理论有效地描述了MIPS系统中的界面动态与气泡.
- 有效的表面张力可以从蒸汽密度的变化中推断出来,量化波动.
- 与平衡系统相比,非平衡液相表现出明显的波动特征.
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