文摘
Solutions of P-SV equations of motion in a homogeneous transversely isotropic elastic layer contain a factor exp(±νjz), where z is the vertical coordinate and j = 1, 2. For computing Rayleigh wave dispersion in a multi-layered half space, νj is computed at each layer. For a given phase velocity (c), νj becomes complex depending on the transversely isotropic parameters. When νj is complex, classical Rayleigh waves do not exist and generalised Rayleigh waves propagate along a path inclined to the interface. We use transversely isotropic parameters as αH, βV, ξ, ϕ and η and find their limits beyond which νj becomes complex. It is seen that νj depends on ϕ and η, but does not depend on ξ. The complex νj occurs when ϕ is small and η is large. For a given c/βV, the region of complex νj in a ϕ -η plane increases with the increase of αH/βV. Further, for a given αH/βV, the complex region of νj increases significantly with the decrease of c/βV. This study is useful to compute dispersion parameters of Rayleigh waves in a layered medium.