The rotlet is the point-torque fundamental solution of Stokes flow. Its torque strength is an axial vector, and its circulating velocity decays as . A freely swimming cell with no external torque is torque-free. The motor applies opposite internal torques to its body and flagellar apparatus, so the net torque monopole satisfies
Individual body and flagellar torques need not vanish. A spatially separated pair can therefore leave a rotlet dipole even though there is no far-field rotlet monopole.

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