Abstract

Locally resonant acoustic metamaterial (LRAM) panels are excellent candidates for the low-frequency flexural wave attenuation in thin structures. To enable the efficient analysis and design of LRAM beam/shell structural elements for practical applications, a computational homogenization method for modelling wave propagation phenomena in LRAM panels is presented in this work. The approach is based on the notion of a relaxed separation of scales, which tailors the methodology to the phenomena governed by local resonators embedded in a host medium. The macroscopic LRAM panel is modelled as a thin continuum beam/shell described by proper structural kinematics and momentum balance relations. At the microscale, a LRAM unit cell is considered with lamina-wise in-plane boundary conditions and zero out-of-plane tractions, representing the free top and bottom surfaces of the macroscopic LRAM panel. Under the assumption of linear elasticity, in the relaxed separation of scales regime, the microscale unit cell problem can be represented by the superposition of a static and a dynamic problem, hereby enabling a significant model reduction. As a result, the macroscale effective material properties can be computed once and for all off-line for a given unit cell. In addition, a new macroscale evolution equation emerges describing the effect of the microscale internal dynamics on the macroscopic fields through the introduction of new macroscale enrichment variables, which reflect the modal amplitudes of localized microscale modes. The proposed homogenization methodology reveals a high level of accuracy and numerical efficiency compared to the reference direct numerical simulation (DNS) for all relevant analyses: computation of real and complex dispersion spectra for an infinite LRAM panel, as well as steady-state frequency response and transient behaviour for a finite LRAM panel.

Highlights

  • Along with the growing environmental and economic requirements, lighter, and stronger, designs are being constantly pursued in modern society [1]

  • The macroscopic Locally resonant acoustic metamaterial (LRAM) panel is modelled as a thin continuum beam/shell described by proper structural kinematics and momentum balance relations

  • A LRAM unit cell is considered with lamina-wise in-plane boundary conditions and zero out-of-plane tractions, representing the free top and bottom surfaces of the macroscopic LRAM panel

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Summary

Introduction

Along with the growing environmental and economic requirements, lighter, and stronger, designs are being constantly pursued in modern society [1]. It must be pointed out that these dynamic computational homogenization frameworks are developed using a classical continuum solid description at both micro and macroscales As a result, they may not be directly applied to study thin LRAM panels with the (mostly) single-layer configurations, (approximately) free top and bottom surfaces, and (possibly) simultaneous coupled propagation of both body and flexural waves. Combining this reduced unit cell model with the upscaling relations, yields the enriched macroscopic continuum beam/shell description. The subscript “M” is temporarily omitted since only one (macro) scale is relevant here

Kinematics
Stress and momentum resultants
Weak and strong forms of the balance equations
Microscale: continuum solid description
Separation of scales
Dynamic computational homogenization framework for LRAM panels
Macro-to-micro scale transition
Micro-to-macro scale transition
Finite element discretization of the microscale problem
Static-dynamic decomposition and model reduction
Internal dynamics
Homogenized constitutive relations
Summary of the reduced homogenization framework
Numerical simulations on an infinite LRAM panel
Dispersion relation
Case study of an infinite LRAM panel
Numerical simulations on a finite LRAM panel
Method
Steady-state frequency response analysis
Transient analysis
Computational costs
Findings
Conclusions

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