Abstract

We investigate theoretically and experimentally the forced response of flexural waves propagating in a 1D phononic crystal (PC) Euler-Bernoulli beam, composed by steel and polyethylene, and its band structure. The finite element, spectral element, wave finite element, wave spectral element, conventional and improved plane wave expansion methods are applied. We demonstrate that the vibration attenuation of the unit cell can be improved choosing correctly the polyethylene and steel quantities and we suggest the best percentages of these materials, considering different unit cell lengths. An experiment with a 1D PC beam is proposed and the numerical results can localize the band gap position and width close to the experimental results. A small Bragg-type band gap with low attenuation is observed between 405 Hz - 720 Hz. The 1D PC beam with unit cells of steel and polyethylene presents potential application for vibration control.

Highlights

  • Artificial periodic composites known as phononic crystals (PCs), consisting of a periodic array of scatterers embedded in a host medium, have been quite studied[1,2,3,4,5,6,7,8,9,10,11,12,13,14]

  • The main purpose of this study is to investigate the Bragg-type band gap formation, band structure, known as dispersion relation, and attenuation constant of a 1D PC beam using the FE, SE, wave finite element (WFE), wave spectral element (WSE), conventional plane wave expansion (CPWE) and improved plane wave expansion (IPWE) methods

  • We obtain the forced response and the complex elastic band structure of a 1D PC beam proposed by models 1 and 2

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Summary

Introduction

Artificial periodic composites known as phononic crystals (PCs), consisting of a periodic array of scatterers embedded in a host medium, have been quite studied[1,2,3,4,5,6,7,8,9,10,11,12,13,14]. They have received renewed attention because they exhibit band gaps where there are only mechanical (elastic or acoustic) evanescent waves. PCs have many applications, such as vibration isolation technology[16,17,18,19,20], acoustic barriers/filters[21,22,23], noise suppression devices[24,25], surface acoustic devices[26], architectural design[27], sound shields[28], acoustic diodes[29] and elastic/acoustic metamaterials[19,20,23,25,30,31,32] (EM/AM), known as locally resonant phononic crystals (LRPC)

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