Going in circles: Slender body analysis of a self-propelling bent rod

We study the two-dimensional motion of a self-propelling asymmetric bent rod. By employing slender body theory and the Lorentz reciprocal theorem, we determine particle trajectories for different geometric configurations and arbitrary surface activities. Our analysis reveals that all particle trajectories can be mathematically expressed through the equation for a circle. The rotational speed of the particle dictates the frequency of the circular motion and the ratio of translational and rotational speeds describes the radius of the circular trajectory. We find that even for uniform surface activity, geometric asymmetry is sufficient to induce a self-propelling motion. Specifically, for uniform surface activity, we observe (i) when bent rod arm lengths are equal, the particle only translates, (ii) when the length of one arm is approximately four times the length of the other arm and the angle between the arms is approximately pi 2 , the rotational and translational speeds are at their maximum. We explain these trends by comparing the impact of geometry on the hydrodynamic resistance tensor and the active driving force. Overall, the results presented here quantify self-propulsion in composite-slender bodies and motivate future research into self-propulsion of highly asymmetric particles.

Automated summary

We study the 2D motion of a self-propelling asymmetric bent rod and find that all particle trajectories can be mathematically expressed through the equation for a circle. The rotational speed of the particle determines the frequency of circular motion, while the ratio of translational and rotational speeds describes the radius of the circular trajectory. Our analysis shows that even with uniform surface activity, geometric asymmetry is enough to induce self-propulsion. The results provide insights into the self-propulsion of highly asymmetric particles.