We show that an energy decay \\u(t)\\(2) = 0(t(-mu)) for Solutions of the Navier-Stokes equations on R(n), n less than or equal to 5, implies a decay of the higher order norms, e.g. \\D(alpha)u(t)\\(2) = O(t(-mu-\alpha\/2)) and \\u(t)\\(infinity) = O(t(-mu-mu/4)).