“…In this problem, Ω := (0, 1)×(0, 1 4 ), 1 4 ], Γ t := [1, 0] × { 1 4 }, Γ l := {0} × [ 1 4 , 0], f = 0, u = 0 on Γ b ∪ Γ r ∪ Γ l , ∂u ∂y + iku = g t on Γ t , which is the lowest-order approximation of the radiation boundary condition (see [6,18]). Setting g t = -2ik cos θ e ik sin θx and θ = π 4 (see [6,36]), we show that the real part, the image part and magnitude of the solution with k = 128π, N = 512 in Figs. 3-4, which is consistent with that illustrated in [6,36].…”