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Coherent waves in a multiply scattering poro-elastic medium obeying Biot's theory

机译:遵循比奥特理论的多重散射多孔弹性介质中的相干波

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Twersky's theory is generalized to multiple scattering by a uniform random distribution of cylinders in a poro-elastic medium. The high-frequency regime only, where no dispersion effects occur in the absence of scatterers, is investigated in the frame of Biot's theory. The scatterers lie within a slab of the host medium, and an incident wave gives rise to a fast longitudinal coherent wave, a slow longitudinal one, as well as a shear one in the slab. The dispersion equations of those three coherent waves are derived. The shear coherent wave propagates independently of the other two, while the longitudinal coherent waves obey a coupled dispersion equation involving conversion terms. Numerically speaking, coupling effects are significant only when forward scattering by a single cylinder of the fast wave into the slow one (or the slow wave into the fast) is larger than forward scattering with no conversion.
机译:Twersky的理论通过在弹性弹性介质中圆柱体的均匀随机分布而推广到多重散射。仅在高频状态下,在没有散射体的情况下不会发生色散效应,这是在毕奥特理论的框架内进行的。散射体位于宿主介质的平板中,入射波在平板中产生快速的纵向相干波,缓慢的纵向相干波和剪切波。推导了这三个相干波的色散方程。剪切相干波独立于其他两个相干传播,而纵向相干波服从包含转换项的耦合色散方程。从数值上讲,仅当单个波的快波向慢波(或慢波向快波)的向前散射大于没有转换的正向散射时,耦合效应才有意义。

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