“…If ( u , p ) satisfies W1 , then ( , , { σ (u, p )n jm } m ∈ N ( j ) ) is also solution of the local problem W2 , for every j = 1, …, N Ω . The Lagrange multipliers therefore play the role of the stress at the interfaces; for details, see, e.g., [ 25 , 43 ]. Conversely, if ( u j , p j , { λ [ jm ] } m ∈ N ( j ) ) are the local solutions of W2 , then is solution of W1 .…”