Enforcing angular-momentum conservation without stress symmetry yields a 2D chiral hydrodynamics in which every odd channel is the 90° rotation of a Newtonian one, and confined steady flows reduce to a modified Helmholtz–Poisson cavity controlled by a single group αL.
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Steady base states in a two-dimensional chiral fluid. The chiral Stokes cavity
Enforcing angular-momentum conservation without stress symmetry yields a 2D chiral hydrodynamics in which every odd channel is the 90° rotation of a Newtonian one, and confined steady flows reduce to a modified Helmholtz–Poisson cavity controlled by a single group αL.