Abstract

Classically, the rotation of ellipsoids in shear Stokes flow is captured by Jeffery's orbits. Here, we demonstrate that Jeffery's orbits also describe high-frequency shape-deforming swimmers moving in the plane of a shear flow. In doing so, we support the use of these simple models for capturing shape-changing swimmer dynamics in studies of active matter and highlight the ubiquity of ellipsoid-like dynamics in complex systems.

Highlights

  • [22] In writing this, we are minimally abusing notation by interpreting xS as a two-dimensional vector field in order to write the scalar product between it and LU r, which we will continue to do throughout, noting that this is unambiguous as xS · ez ≡ 0

  • A similar correspondence holds between rigid bodies and ellipsoids in Stokesian fluid dynamics, with the angular motion of a broad class of particles in shear flow known to be equivalent to those of an ellipsoid

  • Though we have focused on the motion of rapidly deforming swimmers, Eq (4) can be further analysed in two additional cases: slow swimmer evolution, where ω 1, and a rigid body, where ω = 0 and T is constant

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Summary

Introduction

[22] In writing this, we are minimally abusing notation by interpreting xS as a two-dimensional vector field in order to write the scalar product between it and LU r, which we will continue to do throughout, noting that this is unambiguous as xS · ez ≡ 0. The rotation of ellipsoids in shear Stokes flow is captured by Jeffery’s orbits.

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