毛细血管张力理论和运动诱导相位的界面动力学
Luke Langford1, Ahmad K Omar1,2
1Department of Materials Science and Engineering, <a href="https://ror.org/01an7q238">University of California, Berkeley</a>, California 94720, USA.
这项研究引入了远离平衡的接口的新理论,定义了一种新的"活性表面张力",它控制了时间逆向对称性破碎的系统中的接口动力学.
科学领域:
- 统计力学 统计力学
- 软物质物理学 软物质物理学
- 活体物质系统是什么
背景情况:
- 平衡界面的统计力学已经很成熟.
- 最近的观察强调了对远离平衡的接口需要新的理论.
- 现有的理论无法充分描述破坏时间逆转对称性的系统.
研究的目的:
- 从微观粒子动力学中推导出共存的运动诱导相的线性界面动力学.
- 为了确定控制界面波动的热能量尺度和不平衡表面张力.
- 在平衡系统中区分主动表面张力和机械表面张力.
主要方法:
- 从破碎时间逆向对称的微观粒子动力学得出的推导.
- 在共存的运动诱导相中分析线性界面动力学.
- 与现有的模拟数据和理论框架进行比较 (例如,Kirkwood-Buff).
主要成果:
- 识别一种热能尺度激发界面波动.
- 定义一个不平衡的表面张力,不同于机械的表面张力,可以抑制波动.
- 证明表面刚度与粒子持久长度线性变化.
- 确认接口服从表面积,最大限度地减少波兹曼统计在大波长.
结论:
- 为不平衡界面建立了一个新的理论框架.
- 由非保守力引起的活性表面张力,在活性物质系统中起着关键作用.
- 衍生理论与模拟数据保持一致,并将平衡概念扩展到远离平衡的制度.
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