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Reflection, transmission and excitation of SH-surface waves by a discontinuity in mass-loading on a semi-infinite elastic medium
Authors:D Quak and F L Neerhoff
Institution:(1) Dept. of Elect. Eng., Div. of Electromagnetic Res., Delft Univ. of Technology, Delft, The Netherlands
Abstract:The scattering of an SH-wave by a discontinuity in mass-loading on a semi-infinite elastic medium is investigated theoretically. The incident wave is either a plane body wave or a plane SH-surface wave. The problem is reduced to a Wiener-Hopf problem for the scattered wave. In this problem the amplitude spectral density of the particle displacement occurs as unknown function. Special attention is given to the numerical values of the surface wave contributions to the scattered field.Nomenclature x 1, x 2, x 3 Cartesian coordinates - gamma, chi polar coordinates in x 1, x 3-plane - rgr volume mass density - sgr surface mass density of mass-loading - lambda, mgr Lamé constants - U scalar wave function, defined by (2.1) - c S speed of propagation of uniform shear waves in bulk medium (c S=(mgr/rgr)1/2) - ohgr angular frequency - t time - k S wave number of uniform shear waves (k S=ohgr/c S) - eegr reduced specific acoustic impedance of mass-loading (eegr=k S sgr/rgr) - k m wave number of SH-surface wave (k m=k S(1+eegr 2)1/2) - part 1,2,3 partial differentiation with respect to x 1,2,3 - theta i angle between x 3-axis and direction of propagation of incident body wave - agr i wave number in horizontal direction of incident body wave (agr i=k S sin(theta i)) - gamma i wave number in vertical direction of incident body wave (gamma i=k S cos(theta i)) - C 1,2 complex amplitude of surface wave excited by a body wave - R reflection factor of surface wave, when surface wave is incident - T transmission factor of surface wave, when surface wave is incident - S particle displacement vector The research presented in this paper has been carried out with partial financial support from the Delfts Hogeschoolfonds.
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