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Taylor's chiral microswimmer
Phys. Rev. Fluids 8, 044201 – Published 28 April, 2023
DOI: https://doi.org/10.1103/PhysRevFluids.8.044201
Abstract
In order to understand the rotational motion of a microswimmer in a Newtonian fluid, we model it as an infinite cylinder with a helical, propagating surface wave. Using the method of series expansion, we calculate the linear and angular velocities of the cylinder, assuming that the wave amplitude is much smaller than the wavelength. To the first order in the wave amplitude, for the first mode of a purely azimuthal wave (that is, when the wavelength equals the cylinder's circumference), the cylinder moves along a circular path in the plane normal to its axis. Otherwise, the first-order velocities of the cylinder are zero, like the Taylor sheet. The time-averaged motion of the cylinder is determined by calculating the second-order velocities; the axial component of the wave vector leads to the linear motion of the cylinder along its axis and the azimuthal component to the angular motion around the axis. With the same stroke, the cylinder is always slower and less efficient than the Taylor sheet.
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