Motion characteristics of squirmers in linear shear flow

IF 1.3 4区 工程技术 Q3 MECHANICS
Geng Guan, Yuxiang Ying, Jianzhong Lin, Jue Zhu
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Abstract

In this study, the two-dimensional lattice Boltzmann method was employed to simulate the motions and distributions of a circular squirmer in a linear shear flow. The objective was to systematically investigate the dynamics of microorganisms or engineered squirmers in a flowing environment. We conducted multiple simulations across a range of self-propelled strengths (0.08 ⩽ α ⩽ 0.8) and squirmer type parameters (−5 ⩽ β ⩽ 5). Initially, we analyzed the swimming motions of the neutral squirmer (β = 0) in the shear flow. Our analysis revealed two distinct distributions depending on α, i.e. near the bottom or the top plate, which differs from conventional particle behavior. Moreover, we observed that the separation point of these two distributions occurs at αc = 0.41. The puller and pusher exhibit similarities and differences, with both showing a periodic oscillation pattern. Additionally, both types reach a steady inclined pattern near the plate, with the distinction that the low-pressure region of the puller’s head is captured by the plate, whereas the pusher is captured by the low-pressure region on the side of the body. The limit cycle pattern (LCP) is unique to the pusher because the response of the pressure distribution around the pusher to the flow field is different from that of a puller. The pusher starts from the initial motion and asymptotes to a closed limit cycle under the influence of flow-solid interaction. The frequency St of LCP is inversely proportional to the amplitude h * because the pusher takes longer to complete a larger limit cycle. Finally, an open limit cycle is shown, representing a swimming pattern that crosses the width of the channel.
线性剪切流中蠕动器的运动特性
本研究采用二维晶格玻尔兹曼法模拟了线性剪切流中圆形蠕虫的运动和分布。目的是系统地研究流动环境中微生物或工程蠕虫的动力学。我们在一定范围的自推进强度(0.08 ⩽ α ⩽ 0.8)和蠕动器类型参数(-5 ⩽ β ⩽ 5)下进行了多次模拟。最初,我们分析了中性松鼠(β = 0)在剪切流中的游泳运动。我们的分析发现,根据 α 的不同,有两种截然不同的分布,即靠近底板或顶板,这与传统的粒子行为不同。此外,我们观察到这两种分布的分离点出现在 αc = 0.41 处。拉力器和推力器有相似之处,也有不同之处,两者都呈现周期性振荡模式。此外,两种类型都在板附近达到稳定的倾斜模式,区别在于拉杆头部的低压区被板捕获,而推杆则被杆身一侧的低压区捕获。极限循环模式(LCP)是推杆所特有的,因为推杆周围的压力分布对流场的响应不同于拉杆。推杆从初始运动开始,在流固相互作用的影响下渐近于一个封闭的极限循环。LCP 的频率 St 与振幅 h* 成反比,因为推杆需要更长的时间才能完成较大的极限循环。最后,图中显示的是一个开放式极限循环,代表一种横跨通道宽度的游动模式。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Fluid Dynamics Research
Fluid Dynamics Research 物理-力学
CiteScore
2.90
自引率
6.70%
发文量
37
审稿时长
5 months
期刊介绍: Fluid Dynamics Research publishes original and creative works in all fields of fluid dynamics. The scope includes theoretical, numerical and experimental studies that contribute to the fundamental understanding and/or application of fluid phenomena.
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