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Elastodynamics of radially inhomogeneous spherically anisotropic elastic materials in the Stroh formalism

机译:Stroh形式主义中径向非均匀球形各向异性弹性材料的弹性动力学

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摘要

A method for solving elastodynamic problems in radially inhomogeneous elastic materials with spherical anisotropy is presented, i.e. materials having c _(ijkl)= c _(ijkl)(γ) in a spherical coordinate system {γ,θ, φ}. The time-harmonic displacement field u(γ,θ, φ) is expanded in a separation of variables form with dependence on θ, φ described by vector spherical harmonics with γ-dependent amplitudes. It is proved that such separation of variables solution is generally possible only if the spherical anisotropy is restricted to transverse isotropy (TI) with the principal axis in the radial direction, in which case the amplitudes are determined by a first-order ordinary differential system. Restricted forms of the displacement field, such as u(θ, φ), admit this type of separation of variables solution for certain lower material symmetries. These results extend the Stroh formalism of elastodynamics in rectangular and cylindrical systems to spherical coordinates.
机译:提出了一种解决具有球形各向异性的径向非均质弹性材料中弹性力学问题的方法,即在球坐标系{γ,θ,φ}中具有c _(ijkl)= c _(ijkl)(γ)的材料。时谐位移场u(γ,θ,φ)扩展为变量形式的分离,该变量形式取决于矢量球谐函数描述的θ,φ,且振幅取决于γ。事实证明,只有当球形各向异性被限制为主轴方向为径向的横向各向同性(TI)时,这种变量解的分离通常是可能的,在这种情况下,振幅是由一阶常微分系统确定的。位移场的限制形式(例如u(θ,φ))允许对于某些较低的材料对称性使用这种类型的变量解分离。这些结果将矩形和圆柱系统中的弹性动力学的Stroh形式主义扩展到了球形坐标。

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