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This research article explores the phenomena of the reflection and refraction of plane waves at two interfaces, one of which is the interface between the micropolar elastic solid half-space and viscous liquid layer and another interface between the inviscid liquid half-space and viscous liquid layer. The basic equations of micropolar elastic solids and viscous and inviscid liquids are converted into the xy-plane and solved with the plane harmonic solution method. On the plane interfaces, the primary wave (P-wave) or vertical shear wave (SV-wave) is considered to be an incident wave. The sliding contact parameter-influenced reflected waves in a micropolar elastic solid half-space, and the refracted waves in a viscous liquid layer are derived analytically. In micropolar elastic solids, there are three different kinds of waves named P-wave, SV-wave, and microrotational wave (MR-wave), each with different speeds. P-waves and SV waves are present in viscous liquids, while SV waves are present in inviscid liquid half-spaces. Thickness-influenced amplitude ratios are obtained at the interface boundary between the viscous liquid layer and the inviscid liquid half-space, whereas sliding contact parameter-influenced amplitude ratios are obtained at the interface boundary between the micropolar elastic solid half-space and the viscous liquid layer. The detailed study on the impacts of the sliding contact parameter and the thickness of the viscous liquid layer is presented graphically for a particular model.
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Kamidi et al. (2026) studied this question.
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