Setter E, Bucher I, Haber S
Faculty of Mechanical Engineering, Technion-Israel Institute of Technology, Haifa 32000, Israel.
Phys Rev E Stat Nonlin Soft Matter Phys. 2012 Jun;85(6 Pt 2):066304. doi: 10.1103/PhysRevE.85.066304. Epub 2012 Jun 5.
Microscale slender swimmers are frequently encountered in nature and are now used in microrobotic applications. The swimming mechanism examined in this paper is based on small transverse axisymmetric traveling wave deformations of a cylindrical long shell. The thin-shelled device is assumed to be inextensible at the middle surface and extensible at the surface wetted by the fluid. Assuming low-Reynolds-number hydrodynamics, an analytical solution is derived for waves of small amplitudes compared with the cylinder diameter. We show that swimming velocity increases with β(1) (the ratio of cylinder radius to wavelength) and that swimming velocity is linearly dependent on wave propagation velocity, increasing to leading order with the square of the ratio of wave amplitude to wavelength β(2) and decreasing with the wall thickness. A fourth-order correction in β(2) was also calculated and was found to have a negative effect on the swimming velocity. The results for a shell of negligible-wall thickness were compared with Taylor's solution for an inextensible two-dimensional flat membrane undergoing a waving motion and Felderhof's results [Phys. Fluids 22, 113604 (2010)] for an unbounded flow field and negligible-wall thickness. We show that Taylor's analytic solution is a particular limiting case of the present solution, assuming zero wall thickness and infinite values of β(1). The present mechanism was also compared with Taylor's well known solutions of waving planar and helical circular tails. We show that the present approach yields higher velocities as β(1) increases, whereas, the opposite occurs for waving tails. Indeed, in the region where β(1)>15, the present approach yields velocities nearly as fast as Taylor's helical waving tail while consuming less power and with a design that is considerably more compact. In this regime, the axisymmetric swimmer is twice as fast as Taylor's planar-tail swimmer for an additional investment of only one-third of the power. Experiments were conducted using a macroscale autonomous model immersed in highly viscous silicone fluid. We outlined how the proposed mechanism was realized to propel an elongated, yet finite, swimmer. Measured data demonstrate the effects of wave velocity and wavelength on swimming speed, showing good agreement with analytical results.
微尺度细长型游动体在自然界中经常出现,目前被应用于微型机器人领域。本文所研究的游动机制基于圆柱形长壳体的小横向轴对称行波变形。该薄壳装置假定在中面不可伸长,而在被流体浸湿的表面可伸长。假设流体动力学为低雷诺数,针对与圆柱直径相比振幅较小的波,推导了一个解析解。我们表明,游动速度随β(1)(圆柱半径与波长之比)增加,且游动速度与波传播速度呈线性相关,随波幅与波长之比β(2)的平方呈一阶增加,并随壁厚减小。还计算了β(2)的四阶修正,发现其对游动速度有负面影响。将壁厚可忽略不计的壳体结果与泰勒关于不可伸长二维平面膜做波动运动的解以及费尔德霍夫关于无界流场且壁厚可忽略不计的结果[《物理流体》22, 113604 (2010)]进行了比较。我们表明,假设壁厚为零且β(1)为无穷大时,泰勒的解析解是本文解的一个特殊极限情况。还将本文机制与泰勒著名的波动平面尾和螺旋圆形尾的解进行了比较。我们表明,随着β(1)增加,本文方法产生的速度更高,而对于波动尾则相反。实际上,在β(1)>15的区域,本文方法产生的速度几乎与泰勒的螺旋波动尾一样快,同时消耗的功率更少且设计更为紧凑。在这种情况下,轴对称游动体速度是泰勒平面尾游动体的两倍,而额外消耗的功率仅为其三分之一。使用浸没在高粘性硅酮流体中的宏观自主模型进行了实验。我们概述了如何实现所提出的机制以推动一个细长但有限的游动体。测量数据展示了波速和波长对游动速度的影响,与解析结果吻合良好。