AbstractThe Helmholtz Equation (− Δ − K2n2)u = 0 with a variable index of refraction, n, and a suitable radiation condition at infinity serves as a model for a wide variety of wave propagation problems. A numerical algorithm has been developed and a computer code implemented that can effectively solve this equation in the intermediate frequency range. The equation is discretized by using the finite element method, thus allowing for the modeling of complicated geometries (including interfaces) and complicated boundary conditions. A global radiation boundary condition is imposed at the far-field boundary that is exact for an arbitrary number of propagating modes.The resulting large, nonselfadjoint system of linear equations with indefinite sy...