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    Hamiltonian formulation for the motion of an active spheroidal particle suspended in laminar straight duct flow

    Brendan Harding*

    Rahil N. Valani†

    Yvonne M. Stokes‡

    • *Contact author: brendan.harding@vuw.ac.nz
    • †Contact author: rahil.valani@physics.ox.ac.uk
    • ‡Contact author: yvonne.stokes@adelaide.edu.au

    Phys. Rev. E 112, 054125 – Published 17 November, 2025

    DOI: https://doi.org/10.1103/m9ks-mq3d

    Abstract

    We analyze a generalization of Zöttl and Stark's model of active spherical particles [Phys. Rev. Lett. 108, 218104 (2012)] and prolate spheroidal particles [Eur. Phys. J. E 36, 4 (2013)] suspended in cylindrical Poiseuille flow, to particle dynamics in an arbitrary unidirectional steady laminar flow through a straight duct geometry. Our primary contribution is to describe a Hamiltonian formulation of these systems and provide explicit forms of the constants of motions in terms of the arbitrary fluid velocity field. The Hamiltonian formulation provides a convenient and robust approach to the computation of particle orbits while also providing new insights into the dynamics, specifically the way in which orbits are trapped within basins defined by a potential well. In addition to considering spherical and prolate spheroidal particles, we also illustrate that the model can be adapted to oblate spheroidal particles.

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