For the two dimensional stationary MHD equations, we prove that Liouville type theorems hold if the velocity is growing at infinity, where the magnetic field is assumed to be bounded under a smallness condition. The key point is to overcome the nonlinear terms, since no maximum principle holds for the MHD case with respect to the Navier-Stokes equations. As a corollary, we obtain that all the solutions of the 2D Navier-Stokes equations satisfying ∇u ∈ L p (R 2 ) with 1 < p < ∞ are constants, which is sharp since the same argument fails in the case of ∇u ∈ L ∞ (R 2 ).