For rigid fluidrotation with vorticity−2Ωe2, BΩ≫1, and BDR of order one, the normalized steady density is f=(4π)−1[1−2p1/(BΩ)]+O((BΩ)−2). The result follows by acting with the rotation generator on p1 and using ∫pipjdΩ=4πδij/3. Reversing the imposed rotation reverses the mean horizontal swimming direction.