椭圆截面微通道中活性棒的边界积聚

Chase Brown, Mykhailo Potomkin, Shawn Ryan
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摘要

许多运动微生物和生物仿真微粒都被成功地模拟为活动杆--能够自我推进的细长体。在封闭条件下,主动杆动力学的一个特点是它们倾向于在壁上聚集。被动粒子通常会在壁面沉积并停止运动,而积聚的主动杆则不同,它们会继续沿壁面运动、调整方向,甚至可能从壁面逃逸。活性棒在壁面和远离壁面时的动态变化导致了复杂的非三维分布。在这项工作中,我们通过研究管状微通道的椭圆扰动,即自然界和各种应用中常见的横截面为圆形的圆柱形封闭,来考察管壁曲率对活性棒分布的影响。通过建立单个活性棒的计算模型并进行蒙特卡洛模拟,我们发现活性棒往往集中在管壁曲率最大的位置。然后,我们研究了活性棒积聚的分布如何取决于背景流和取向扩散。最后,我们用一个简化的数学模型解释了为什么活性棒优先聚集在高曲率位置。
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Boundary accumulations of active rods in microchannels with elliptical cross-section
Many motile microorganisms and bio-mimetic micro-particles have been successfully modeled as active rods - elongated bodies capable of self-propulsion. A hallmark of active rod dynamics under confinement is their tendency to accumulate at the walls. Unlike passive particles, which typically sediment and cease their motion at the wall, accumulated active rods continue to move along the wall, reorient, and may even escape from it. The dynamics of active rods at the wall and those away from it result in complex and non-trivial distributions. In this work, we examine the effects of wall curvature on active rod distribution by studying elliptical perturbations of tube-like microchannels, that is, the cylindrical confinement with a circular cross-section, common in both nature and various applications. By developing a computational model for individual active rods and conducting Monte Carlo simulations, we discovered that active rods tend to concentrate at locations with the highest wall curvature. We then investigated how the distribution of active rod accumulation depends on the background flow and orientation diffusion. Finally, we used a simplified mathematical model to explain why active rods preferentially accumulate at high-curvature locations.
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