“…3 := {φ ∈ D(Ω) 3 : v is equal to 0 in a neighbourhood of Γ 1 }, w 0 , w 1 , v 0 ∈ [D(Ω)] 3 , ψ 0 (x) = ψ 0 x ε with ψ 0 ∈ H 1 (Y 0 ) 3 (Y-periodically extended to R 3 ), ψ 1 (x) = ψ 1 x ε with ψ 1 ∈ H 1 per (Y 1 ) 3 such that ∇ × ϕ ε 0 = 0. Then, ϕ ε ∈ W d (Ω ε ),…”