活性颗粒与半柔性聚合物网络结合的不平衡扩散:模拟和分数朗格温方程
Hyeong-Tark Han1, Sungmin Joo1, Takahiro Sakaue2
1Department of Physics, POSTECH, Pohang 37673, Republic of Korea.
The Journal of chemical physics
|July 10, 2023
概括
粘弹性介质中的自推粒子表现出复杂的扩散. 这项研究揭示了由导线相互作用控制的活性粘弹性动力学,显示了由超扩散到亚扩散的过渡取决于推进强度和时间.
科学领域:
- 软物质物理学 软物质物理学
- 活动物质 活动物质
- 生物物理学的生物物理.
背景情况:
- 粘弹性环境中的粒子扩散是由于记忆效应而非马科维的.
- 在这种介质中理解自行推进粒子扩散与定向记忆仍然是一个开放的问题.
研究的目的:
- 量化解释在粘弹性介质中具有方向记忆的自我推进粒子的扩散.
- 为了研究由半柔性纤维连接的颗粒的活性粘弹性系统.
主要方法:
- 兰杰文动力学模拟.
- 分析理论. 分析理论.
- 分数兰杰文方程建模.
主要成果:
- 活性粒子具有依赖时间的异常扩散 (超扩散和亚扩散),指数为α.
- 短时间的超扩散 (α=3/2) 过渡到较长时间的亚扩散 (1/2 ≤ α ≤ 3/4).
- 活跃的亚扩散被强烈的推进 (Pe) 增强,可能模仿高Pe的Rouse运动.
结论:
- 半柔性丝网中的活性粒子运动可以用分数朗格温方程来描述.
- 活性粘弹性动力学在值Pe (Pe*) 和特定交叉时间 (τ*, τ†) 以上出现.
- 提供了关于细胞内粘弹性环境中的不平衡活性动态的理论见解.
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