“…Corresponding to the slip boundary condition (1.5) for the Euler equations, there are different choices of boundary conditions for the Navier-Stokes equations, one is the mostly-used no-slip boundary condition, i.e., u ε = 0, on Ω (1.6) This Dirichlet type boundary condition was proposed by Stokes ([33]) assuming that fluid particles are adherent to the boundary due to the positive viscosity. Although the well-posedness of the smooth solution to the initial boundary value problem of the Navier-Stokes equations with the no-slip boundary condition can be established quiet easily (at least local in time), the asymptotic convergence of the solution to the corresponding solution of the Euler equations (1.3) with the boundary condition (1.5) as the viscosity coefficient ε tends to zero is one of major open problems except special cases (see [15,29,31,32]) due to the possible appearance of the boundary layers. In general, only some sufficient conditions are obtained for the convergence in L 2 (Ω), see [21,23,38].…”