Ishimoto Kenta, Gaffney Eamonn A
Research Institute for Mathematical Sciences, Kyoto University, Kyoto 606-8502, Japan.
Wolfson Centre for Mathematical Biology, Mathematical Institute, University of Oxford, Oxford OX2 6GG, United Kingdom.
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Dec;88(6):062702. doi: 10.1103/PhysRevE.88.062702. Epub 2013 Dec 2.
The boundary behavior of axisymmetric microswimming squirmers is theoretically explored within an inertialess Newtonian fluid for a no-slip interface and also a free surface in the small capillary number limit, preventing leading-order surface deformation. Such squirmers are commonly presented as abridged models of ciliates, colonial algae, and Janus particles and we investigate the case of low-mode axisymmetric tangential surface deformations with, in addition, the consideration of a rotlet dipole to represent torque-motor swimmers such as flagellated bacteria. The resulting boundary dynamics reduces to a phase plane in the angle of attack and distance from the boundary, with a simplifying time-reversal duality. Stable swimming adjacent to a no-slip boundary is demonstrated via the presence of stable fixed points and, more generally, all types of fixed points as well as stable and unstable limit cycles occur adjacent to a no-slip boundary with variations in the tangential deformations. Nonetheless, there are constraints on swimmer behavior-for instance, swimmers characterized as pushers are never observed to exhibit stable limit cycles. All such generalities for no-slip boundaries are consistent with observations and more geometrically faithful simulations to date, suggesting the tangential squirmer is a relatively simple framework to enable predications and classifications for the complexities associated with axisymmetric boundary swimming. However, in the presence of a free surface, with asymptotically small capillary number, and thus negligible leading-order surface deformation, no stable surface swimming is predicted across the parameter space considered. While this is in contrast to experimental observations, for example, the free-surface accumulation of sterlet sperm, extensive surfactants are present, most likely invalidating the low capillary number assumption. In turn, this suggests the necessity of surface deformation for stable free-surface three-dimensional finite-size microswimming, as previously highlighted in a two-dimensional mathematical study of singularity swimmers [Crowdy et al., J. Fluid Mech. 681, 24 (2011)].
在无惯性牛顿流体中,针对无滑移界面以及处于小毛细数极限下的自由表面,对轴对称微游动蠕动体的边界行为进行了理论探索,同时防止了主导阶表面变形。此类蠕动体通常被视为纤毛虫、群体藻类和雅努斯粒子的简化模型,我们研究了低模式轴对称切向表面变形的情况,此外,还考虑了一个旋转偶极子来代表诸如鞭毛细菌等扭矩驱动的游动体。由此产生的边界动力学简化为攻角和与边界距离的相平面,具有简化的时间反转对偶性。通过稳定不动点的存在证明了在无滑移边界附近的稳定游动,更一般地说,随着切向变形的变化,在无滑移边界附近会出现各种类型的不动点以及稳定和不稳定极限环。然而,游动体行为存在一些限制——例如,被归类为推进器的游动体从未被观察到表现出稳定极限环。所有这些关于无滑移边界的一般性结论与迄今为止的观测结果以及更符合几何实际的模拟结果一致,这表明切向蠕动体是一个相对简单的框架,能够对与轴对称边界游动相关的复杂性进行预测和分类。然而,在存在自由表面且毛细数渐近小、因此主导阶表面变形可忽略不计的情况下,在所考虑的参数空间内未预测到稳定的表面游动。虽然这与实验观测结果形成对比,例如,小体鲟精子在自由表面的聚集,但存在大量表面活性剂,很可能使低毛细数假设无效。反过来,这表明表面变形对于稳定的自由表面三维有限尺寸微游动是必要的,正如之前在奇点游动体的二维数学研究中所强调的[Crowdy等人,《流体力学杂志》681, 24 (2011)]。