“…The second one, Theorem 5, is a L α result, α > 3, which is proved using energy estimates, using arguments from [2,3,22,32,19]. (3), and suppose either the initial data (u 0 , w 0 , h 0 ) ∈ H × L 2 (Ω ) × H and (f , g) ∈ H × L 2 (Ω ) to be sufficiently small or the viscosities µ, ν, ν 2 to be sufficiently large in such a way to assure uniqueness of the solution (v, z, b) for the stationary problem (5). There exist constants C > 0 and M > 0, independent of t, such that…”