In the first part of the paper we study the large‐time behavior of the higher‐order space derivatives of solutions to the Navier‐Stokes equations in ℝ3. Specifically, we show that if w is a nonzero global weak solution to the Navier‐Stokes equations satisfying the strong energy inequality and 0 < α < β < ∞, then there exist C = C(α,β) > 1, δ0 = δ0(α,β) ∈ (0,1) and t0 = t0(α,β) > 0 such that
for every t > t0 and every δ ∈ [0,δ0]. A denotes the Stokes operator and Aβ its powers. In the second part of the paper we derive several consequences of the above inequality concerning the large‐time energy concentration in w; we show, for example, that for any positive ε and α
where a = lim{t → ∞ ||A1/2w(t)||2/||w(t)||2 is a nonnegative real number and F denotes the Fourier transform in L2(ℝ3)3. If 0 < \varepsilonε < a, then