“…in the case of a locally supersonic compressible flow entering the hyperbolic Euler subdomain Ω − , one needs to add the continuity conditions (4.30) to problem (P 0 ) (Theorem 4.2). The corresponding numerical tests presented in [11] show that the approximate solution (c 2 , c 4 ) tends to infinity if (c 2 , c 4 )(0, x 2 , t) = (0, 0), hence this solution does not satisfy the condition c 2,4 (∞, x 2 , t) = 0. Therefore, in this case, the components c 2 and c 4 must vanish identically.…”