Abstract
The solution technique is based on the representation of the plane linear elastodynamic problem by two reduced wave potentials for both, the half-space and the wedge. Following Herrera's theory, appropriate bases of connectivity conditions are adopted for both these regions, which provide a c-complete system of solutions for the problem. Finally, by discretizing the boundary between the half-space and the wedge, as well as the free boundaries of the half-space and the wedge we formally solve the problem in the least-square sense. The resulting formulas, if encoded in a computer program, will yield the amplitudes of the reflected and transmitted surface waves - along the half-space boundary - as well as the amplitude of the newly generated surface wave along the free boundary of the wedge, and scattered fields of the longitudinal and transverse waves in the half-space and the wedge.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
