Abstract A general multiscale framework for the emergent effective elastodynamics of metamaterials
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A general multiscale framework for the emergent effective elastodynamics of metamaterials

机译:通用的多尺度框架,用于超材料的新兴有效弹性动力学

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AbstractThis paper presents a general multiscale framework towards the computation of the emergent effective elastodynamics of heterogeneous materials, to be applied for the analysis of acoustic metamaterials and phononic crystals. The generality of the framework is exemplified by two key characteristics. First, the underlying formalism relies on the Floquet–Bloch theorem to derive a robust definition of scales and scale separation. Second, unlike most homogenization approaches that rely on a classical volume average, a generalized homogenization operator is defined with respect to a family of particular projection functions. This yields a generalized macro-scale continuum, instead of the classical Cauchy continuum. This enables (in a micromorphic sense) to homogenize the rich dispersive behavior resulting from both Bragg scattering and local resonance. For an arbitrary unit cell, the homogenization projection functions are constructed using the Floquet–Bloch eigenvectors obtained in the desired frequency regime at select high symmetry points, which effectively resolves the emergent phenomena dominating that regime. Furthermore, a generalized Hill–Mandel condition is proposed that ensures power consistency between the homogenized and full-scale model. A high-order spatio-temporal gradient expansion is used to localize the multiscale problem leading to a series of recursive unit cell problems giving the appropriate micro-mechanical corrections. The developed multiscale method is validated against standard numerical Bloch analysis of the dispersion spectra of example unit cells encompassing multiple high-order branches generated by local resonance and/or Bragg scattering.
机译: 摘要 本文提出了一种通用的多尺度框架,用于计算异质材料的新兴有效弹性动力学,将其用于声学超材料和声子晶体的分析。该框架的一般性体现在两个关键特征上。首先,潜在的形式主义依靠Floquet-Bloch定理来得出尺度和尺度分离的可靠定义。其次,与大多数依赖于经典体积平均值的均质化方法不同,针对一类特定的投影函数定义了一个广义的均质化算子。这将产生广义的宏观尺度连续体,而不是经典的柯西连续体。这使得(在微晶意义上)能够使布拉格散射和局部共振所产生的丰富的色散行为均匀化。对于任意晶胞,均质化投影函数是使用在选定的高对称点上按所需频率方案获得的Floquet-Bloch特征向量构建的,这有效地解决了主导该方案的出现现象。此外,提出了广义Hill-Mandel条件,以确保均质模型和满量程模型之间的功率一致性。使用高阶时空梯度扩展来定位多尺度问题,从而导致一系列递归晶胞问题,从而给出适当的微机械校正。所开发的多尺度方法已通过标准数值Bloch分析对示例晶胞的色散谱进行了验证,该晶胞包含局部共振和/或布拉格散射产生的多个高阶分支。

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