The problem of scattering of a plane sonic wave from a soft surface with periodic (sinusoidal) unevenness along one direction is examined by means of the Rayleigh plane-wave expansion and the Waterman extinction methods, numerically implemented by Fourier projection and expansion, respectively. The computations are done with real, double-precision, stochastic arithmetic instead of the usual complex, double-precision floating-point arithmetic in order to precisely evaluate the numerical accuracy of the results conditioned by round-off errors. It is shown that the low-order plane-wave coefficients obtained by the Rayleigh and Waterman methods are identical when obtained from matrix systems that are large enough to give ‘‘convergence’’ of these coefficients. For the same matrix size, the higher-order coefficients differ the higher the diffraction order. It is also shown that the Waterman (Fourier-series) computation of the near field is generally meaningful, whereas that of Rayleigh, involving summation of the plane waves is generally meaningless except near the points of the scattering surface first encountered by the incident wave (i.e., those in the valleys when the incident wave comes from below). Low-order plane-wave scattering coefficients, with at least two-to-three-digit accuracy, and which are identical (to this precision) to the plane-wave coefficients computed by the rigorous integral equation method, are obtained by both the Rayleigh and Waterman methods for scattering surfaces with slopes as large as 2.26 when the number of nonevanescent waves is 5. The number of significant digits decreases as the slope increases.
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