Abstract

Existing investigations on imperfect phononic crystal beams mainly concern periodic multi-span beams carrying either one or two channel waves with random or deterministic disorder in span-length. This paper studies the two channel bending waves in phononic crystal beams consisting of many phases of materials with defects introduced as one structural segment having different cross-sectional dimensions or material parameters. The method of reverberation-ray matrix (MRRM) based on the Timoshenko beam theory, which can conduct high-frequency analysis, is extended for the theoretical analysis of dispersion and transmission of bending waves. The supercell technique and the Floquet–Bloch theorem are adopted for modeling the dispersion characteristics, and the whole finite structural model is used to calculate the transmission spectra. Experimental measurements and numerical calculations are provided to validate the displacement transmission obtained by the proposed MRRM, with the effect of damping on transmission spectra being concerned. The high-frequency calculation applicability of the proposed MRRM is also confirmed by comparing the present results with the corresponding ones either using the transfer matrix method (TMM) or MRRM based on Euler—Bernoulli beam theory. The influences of defect size, defect form, and unit-cell number on the transmission spectra and the band structures are discussed. The drawn conclusions may be useful for designing or evaluating the defected phononic crystal beams in bending wave control. In addition, our conclusions are especially potential for identifying the defect location through bending wave signals.

Highlights

  • IntroductionPhononic crystals [1,2,3,4,5], a kind of periodic structure [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18], are materials or structures with spatial periodicities in the form of constituent material phases, geometrical configurations, or boundary conditions

  • It is known that defects in phononic crystals or disorders in periodic structures might lead to wave/vibration localization [5,7,8,13,14,15,16,17,18]

  • Consider the bending waves in a defected bi-coupled phononic crystal beam consisting of n rigidly connected unit cells, as depicted in Figure 1, whose defect is introduced in the { j}th unit cell

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Summary

Introduction

Phononic crystals [1,2,3,4,5], a kind of periodic structure [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18], are materials or structures with spatial periodicities in the form of constituent material phases, geometrical configurations, or boundary conditions They possess frequency bands that can be exploited to control sonic, acoustic, or elastic wave propagation. Related reviews in [5,14,15,16,17,18,19,20,21,22] generally highlighted the localization phenomenon and its relevant factors such as degree of disorder, strength of coupling, frequency, or number of coupling paths.

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