The wave velocity equation has been obtained for a fiber-reinforced layer resting on monoclinic half space. Dispersion occurs when pure plane waves of different wavelengths have different propagation velocities, so that a wave packet of mixed wavelengths tends to spread out in space. 4, the shear wave velocity of the lower medium is not greater than that of the upper medium, and so these models do not meet the necessary conditions for the existence of Love … LOVE WAVE DISPERSION IN HETEROGENEOUS ANISOTROPIC MEDIA* IION L. ANDEKSONf .\n analysis is made of Love-wave propagation in a medium comlxxctl of transverselv isotropic layers. 1935 R. Kakar / Dispersion of Love wave in an isotropic layer sandwiched between orthotropic and prestressed inhomogeneous half-spaces rather in the basis mechanics of faulting. To assess the suitability of this method, it is applied to real data recorded at the geodetic observatory Wettzell (WET) in southeast The evidence is based upon a substantial Love‐Rayleigh discrepancy observed between periods of 40 s and 120 s. An isotropic mantle model clearly fails to explain the observed dispersion curves. Matlab code to calculate Love and Rayleigh wave dispersion, based on SWAMI from Geogia Tech. in the flgure, as shown. dispersive behavior of these waves, could be observed. Therefore using (10) the dispersion equation But!=k is the slope from the origin to the point (k;!) The pro-cedure is described in detail in section 2. Errors, in rigidity (μh), density and thickness of the anisotropic layer, which arise due to the assumption of isotropy of the medium are calculated by numerically analyzing the frequency equation. Now if we substitute C 1 Po wsfo where c is the phase velocity, we have from (11) and from (9) dbBP = 2mW- 1) since ko = @/Po = k$ where k = o/c. However, in the case of Models No. Frequency equation for Love waves, propagating in a transversely isotropic homogeneous layer which is embedded between two isotropic homogeneous half spaces, is obtained. Dispersion of Love waves is studied in a fibre-reinforced layer resting on monoclinic half-space. Given a value of k and its associated value of!, the phase velocity of the wave is!=k. Errors, in rigidity (μ h), density and thickness of the anisotropic layer, which arise due to the assumption of isotropy of the medium are calculated by numerically analyzing the frequency equation. Love wave dispersion curves for Model No. [6] In this study, we try to estimate Love wave dispersion curves using the simple relationship given above. For a given wave frequency, phase velocity of Love waves in all dispersion modes exhibit obvious toward shift as the film thickness decreases or the surface parameters increase. Shear wave velocity ratio curve for Love waves has been shown graphically for fibre reinforced material layer resting on various monoclinic half-spaces. We advance evidence for the existence of seismic anisotropy in the upper mantle beneath Southern Germany from the dispersion of Love and Rayleigh waves. Love wave dispemioa in a laterally heterogemms layer 365 1 + bXg - - 1 + bXg tan fg = J[I -(I +bx,J2 sin’f,] cotfo-Hb and pl(xg) > 0 which is required when b is negative. 3 are presented in Figs 12 and 13. This is the kind of anisotropy which most commonly occurs at the surface of the earth, and in particular is displayed by bedded sediments. DISPERSION p/l 2p/l 3p/l 4p/l 2w0 w k slope = w/k = phase velocity Figure 3 There are various things to note about this flgure: 1. 2 and No. Moreover, there may exist a cut-off frequency in the first mode dispersion below which Love waves will be evanescent in the structure due to surface effects. 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