In this paper we study Liouville properties of smooth steady axially symmetric solutions of the Navier-Stokes equations. First, we provide another version of the Liouville theorem of [14] in the case of zero swirl, where we replaced the Dirichlet integrability condition by mild decay conditions. Then we prove some Liouville theorems under the assumption ura universal constant to be specified. In particular, if ur(r, z) ≥ − 1 r for ∀(r, z) ∈ [0, ∞) × R, then u ≡ 0. Liouville theorems also hold if lim |x|→∞ Γ = 0 or Γ ∈ L q (R 3 ) for some q ∈ [2, ∞) where Γ = ru θ . We also established some interesting inequalities for Ω := ∂z ur −∂r uz r, showing that ∇Ω can be bounded by Ω itself. All these results are extended to the axially symmetric MHD and Hall-MHD equations with u = ur(r, z)er + u θ (r, z)e θ + uz(r, z)ez, h = h θ (r, z)e θ , indicating that the swirl component of the magnetic field does not affect the triviality. Especially, we establish the maximum principle for the total head pressure Φ = 1 2 (|u| 2 + |h| 2 ) + p for this special solution class.