“…with δ ∈ (0, 1), q ≥ 1, q > d − 1, d ∈ {1, 2, 3}, which allowed to show existence of weak solutions with W 1,q+1 regularity in space, and in turn well-posedness of the acoustic-acoustic coupling problem. The case of the acoustic-acoustic coupling, which we are interested in, is modeled by the presence of spatially varying coefficients in the weak form of the equation (1.2) (see [2] for the linear and [4] and [27] for the nonlinear case) as follows: λ(x) (u) 2 φ} dx ds = 0 holds for all test functions φ ∈X, with (u,u)| t=0 = (u 0 , u 1 ), and appropriately chosen test spaceX. In this model b denotes the quotient between the diffusivity and the bulk modulus, while the other coefficients retain their meaning.…”