GNGTS – Atti del 19° Convegno Nazionale / 04.07 G. P. Deidda (1), G. Ranieri (1) and E. Piano (2) (1) (2) D.I.T., Università di Cagliari Libero professionista ESTIMATION OF NEAR-SURFACE SHEAR-WAVE VELOCITY BY A JOINT ANALYSIS OF RAYLEIGH WAVES AND SH-WAVE REFLECTION EVENTS Shear wave velocity is one of the key parameters used to evaluate near-surface stiffness and in general, for measuring low-strain soil elastic behaviour. In geotechnical engineering, it is classically estimated through invasive seismic methods such as cross-hole and down-hole measurements. Since their employment requires the use of boreholes, they do not permit tests to be performed rapidly and at low costs as requested in near-surface investigations. Non-invasive seismic methods (refraction, reflection and surface waves), which are conducted from the free surface, are more advantageous as they offer the possibility of testing larger portions of soil, without the needs of boreholes, and so they are usually more cost-effective. Among these, SH-wave reflection and surface-wave methods seem to be the most interesting since they have the potential to detect a relatively soft layer underlying a stiffer layer – a capability that can not be offered by refraction seismics. The use of Rayleigh waves for characterisation purposes in geotechnical engineering had a strong impulse with the introduction of the Spectral Analysis of Surface Waves (SASW) method (Nazarian et al., 1983; Stokoe and Nazarian, 1983) and a significant advance was made in the last 20 years (e.g., Nazarian and Stokoe, 1984, 1986; Stokoe and Nazarian, 1985; Gabriels et al., 1987; Tokimatsu et al., 1991; Stokoe et al., 1994; Park et al., 1998). Despite the wide success, two critical aspects still remain in the estimation of near-surface shear-wave velocity by inversion of Rayleigh waves: one is the necessity of assuming a consistent soil model constituted by a succession of parallel layers, each one constituted by a homogeneous and isotropic elastic material; the other concerns the non-uniqueness of the solution, which is a major difficulty for every inversion problem. In fact, the inversion process needs a starting hypothesis of stiffness profile and this needs to be chosen carefully because it can strongly influence the final result. Any information about the site, such as interface position or number of layers, is very important to set some constraints on the solution, in order not only to mitigate the non-uniqueness but also to speed up the convergence of the inversion process. This extra information, which is very often achieved from boreholes, can be obtained using SH-wave shallow seismic reflection. When low velocity materials occur (a quite common condition in near surface), the degree of resolution and accuracy associated to SH-wave reflection imaging is certainly sufficient to set an initial well-constrained earth model for the iterative inversion process of surface waves. On that account, to better estimate near-surface shear-wave velocity profiles, we propose a joint analysis of surface-wave (Rayleigh-wave) and SH-wave reflection data. We analysed experimental data from two test sites for which geological information and seismic velocities, obtained from previous surveys, are available. For each test site both surface-wave and SH-wave reflection data were acquired along GNGTS – Atti del 19° Convegno Nazionale / 04.07 the same line. Dispersion curves of Rayleigh waves, obtained from multichannel analysis in the f-k domain, were inverted with several different starting earth models. At first, using no a priori information the initial model was obtained applying the simple inversion procedure of Steady State Rayleigh Waves method (Jones, 1958; 1962). Another model, obtained by time-to-depth conversion of SH-wave stacked section, was then used as an initial guess. Then, inversion results were compared through the analysis of resolution matrices and rms errors associated to the inversion processes. Analysis of the resolution matrix (R) provided an indication of the uniqueness (in an ideal case, if R equals the identity matrix then the calculated solution is the true and unique solution), as well as a measure of how well or poorly the solution was determined. Analysis of rms error, instead, gave information about the effectiveness of the fitting between numerical and experimental data. In all cases, using the seismic depth sections as initial models, inverted earth model solutions were found to have better accuracy and better convergence than all other solutions. Therefore, the proposed joint analysis technique seems to be more effective than the surface waves method alone, as it has the capability to provide more realistic subsurface models. Such capability is surely interesting when geometrical behaviour is also important, as in the case of site effects investigations. REFERENCES Gabriels, P., Snieder, R., and Nolet, G.; In situ measurements of shear-wave velocity in sediments with higher-mode Rayleigh waves. Geophysical Prospecting 35 (2), 187-196. Jones, R.B.; In-situ mesurement of the dynamic properties of soil by vibration method. Geotechnique 8 (1), pp 1-21. Jones, R.B.; Surface wave technique for measuring the elastic properties and thickness of roads: theoretical development. British J. Of Applied Physics 13, pp 21-29. Nazarian, S., Stokoe II, K.H., and Hudson, W.R.; Use of spectral analysis of surface waves method for determination of moduli and thicknesses of pavement systems. Transportation Res. Record No. 930, pp 38-45. 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