Journal
PHYSICS OF FLUIDS
Volume 32, Issue 4, Pages -Publisher
AMER INST PHYSICS
DOI: 10.1063/1.5143372
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Funding
- Natural Science Foundation of China [11625211, 11272310, 11621202, 61603002]
- National University of Singapore [R-265-000-696-133]
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Understanding the propulsion mechanism of swimming microorganisms will facilitate the development of synthetic microswimmers for active cargo deliveries. Herein, we studied, theoretically and numerically, inertialess locomotion of a microswimmer-a spherical body propelled by two symmetrically actuated elastic filaments in the shape of a circular arc at rest, focusing on the effects of their uniform intrinsic curvature (K) over barc. Combining the resistive force theory for viscous flow and Euler-Bernoulli beam theory for elastic filaments, the elasto-hydrodynamics was solved asymptotically. Our theory was verified by simulations using regularized Stokeslets posed on the filament centerlines, with and without considering hydrodynamic interactions (HIs) between the body and filaments. The asymptotic and numerical results showed qualitative agreement. Reasonable quantitative agreement between the asymptotic results and the numerical predictions neglecting body-filament HIs was observed, especially for small |(K) over barc|. However, they deviated quantitatively from the numerical results with body-filament HIs, especially at a large (K) over barc when the HIs became important owing to the short body-filament distance. The propulsive force generated by two arc-shaped filaments significantly depend on their uniform intrinsic curvature (K) over barc. An appreciable increase in the thrust can be achieved by adjusting (K) over barc, which qualitatively confirms and explains the experimentally reported propulsive enhancement facilitated by intrinsically curved appendages [Z. Ye, S. Regnier, and M. Sitti, Rotating magnetic miniature swimming robots with multiple flexible flagella, IEEE Trans. Rob. 30, 3-13 (2014)]. The increase in (K) over barc can even change the sign of the thrust, leading to counter-intuitive, backward propulsion. The flow field reveals the hydrodynamic signature of the swimmer that shifts with time between a neutral swimmer, a pusher, and a puller.
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