Abstract

S U M M A R Y This paper presents the mathematical derivation of an explicit relation for the apparent (or effective) phase velocity of Rayleigh waves in a vertically heterogeneous, isotropic elastic half-space for harmonic excitation. As a kinematical feature, the apparent phase velocity captures the superposition, in a spatial Fourier series, of the individual modes of propagation of Rayleigh waves and describes the speed of propagation of a composite waveform generated by a vertically oscillating point load. The relation, which is a function of the distance from the source, frequency and depth, depends explicitly on the modal phase and group velocities of Rayleigh waves, and their corresponding wavenumbers and eigenfunctions, which can be computed directly from the solution of the Rayleigh-wave eigenproblem. A practical scenario for the application of the notion of apparent Rayleigh-wave phase velocity is the modelling of the dispersion curve in the well-known surface wave measurement methods ‘spectral analysis of surface waves’ (SASW) and ‘multichannel analysis of surface waves’ (MASW). Apart from a theoretical motivation, the availability in surface wave testing of an explicit formula for the calculation of the apparent Rayleigh-wave phase velocity may lead to the development of a new class of inversion algorithms capable of taking into account the influence of all the modes of surface wave propagation. To demonstrate the exactness of the explicit relation, the predicted values of apparent phase velocity are compared to those computed synthetically from a numerical simulation of SASW and MASW testing for three case studies, which show both single as well as multiple mode dominance effects.

Highlights

  • Since the prediction of surface Rayleigh waves by Lord Rayleigh (1887), their conditions of existence and propagation characteristics in elastic solids have been studied in great detail (e.g. Lamb 1904; Knopoff 1952; Achenbach 1984)

  • The explicit relations derived in the previous section for the apparent Rayleigh-wave phase velocity are hereby validated by comparing the predictions of eqs (12a) and (12b) with the dispersion curves computed using synthetic surface wave data generated from a simulation of

  • To compare the apparent Rayleigh-wave phase velocity computed from eqs (12a) and (12b) with the dispersion curves derived from spectral analysis of surface waves’ (SASW) and multichannel analysis of surface waves’ (MASW) testing configurations, three case studies are considered

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Summary

INTRODUCTION

Since the prediction of surface Rayleigh waves by Lord Rayleigh (1887), their conditions of existence and propagation characteristics in elastic solids have been studied in great detail (e.g. Lamb 1904; Knopoff 1952; Achenbach 1984). The authors provided a formal solution for the average apparent phase velocities (radial and vertical components), which is averaged over a range of offsets from a point source Their analytical expressions involve the medium response, phase velocities and amplitude ratios between horizontal and vertical motions of each mode of propagation using the formulae obtained by Harkrider (1964) for the solution of the Rayleigh-wave eigenproblem, which was extended from the theory of Haskell (1953). The availability of our derived explicit, easy-to-implement formula to compute the Rayleigh-wave apparent phase velocity may help to develop algorithms for the measurement and the inversion of surface wave data, which take into account all the modes of propagation.

VA L I DAT IONTH RO UGHNUMERICALMODELLING
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