声子晶体和声学超材料中元adamping的分数阶演算方法

IF 0.7 Q4 MECHANICS
Milan Cajić, Danilo Karličić, Stepa Paunović, S. Adhikari
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引用次数: 6

摘要

声子和声学材料和结构的研究是近十年来从理论物理转向各种工程领域应用的结果。周期性是声子介质的主要特征,由周期性的物质相位、几何形状或边界条件引起,通过频带结构分析了声子介质的传播特性。为了获得这些特性,通常采用广义布洛赫定理来获得粘滞阻尼谐振超材料的色散关系。本文提出了一种新的分析方法来分析分数阶Kelvin-Voigt和Maxwell阻尼模型引入的声子晶体和声学超材料的分数阶阻尼模型。在数值研究中,利用所提出的模型得到的结果与声子晶体和局部共振声学超材料的弹性情况进行了比较,两者的色散曲线存在显著差异。由于分数阶导数阶数和阻尼参数都可以拟合,分数阶麦克斯韦模型更适合描述整个谱的耗散效应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A fractional calculus approach to metadamping in phononic crystals and acoustic metamaterials
Research on phononic and acoustic materials and structures emerged in the recent decade as a result of switching from theoretical physics to applications in various engineering fields. Periodicity is the main characteristic of the phononic medium stemming from periodic material phases, geometry or the boundary condition with wave propagation properties analysed through frequency band structure. To obtain these characteristics, the generalized Bloch theorem is usually applied to obtain the dispersion relations of viscously damped resonant metamaterials. Here we develop a novel analytical approach to analyse the fractionally damped model of phononic crystals and acoustic metamaterials introduced through the fractional-order Kelvin–Voigt and Maxwell damping models. In the numerical study, the results obtained using the proposed models are compared against the elastic cases of the phononic crystal and locally resonant acoustic metamaterial, where significant differences in dispersion curves are identified. We show that the fractional-order Maxwell model is more suitable for describing the dissipation effect throughout the spectrum due to the possibility of fitting both, the order of fractional derivative and the damping parameter.
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来源期刊
CiteScore
0.90
自引率
0.00%
发文量
4
审稿时长
32 weeks
期刊介绍: Theoretical and Applied Mechanics (TAM) invites submission of original scholarly work in all fields of theoretical and applied mechanics. TAM features selected high quality research articles that represent the broad spectrum of interest in mechanics.
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