The propagation of a Stoneley wave through an inclusion near a liquid/solid interface is investigated on the basis of mode theory [Briers et al., J. Acoust. Soc. Am. 95, 1953–1966, 1967–1976 (1994)]. An expression for the phase and amplitude changes of the Stoneley wave is derived and analyzed in the case of a thin (kd≪1) and of a thick (kd≫1) inclusion of arbitrary length (kd is the multiplication of the liquid wave number with the thickness of the inclusion).
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Briers et al. (1997) studied this question.
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