Phononic crystal with low filling fraction and absolute acoustic band gap in the audible frequency range: A theoretical and experimental study

J. O. Vasseur, P. A. Deymier, A. Khelif, Ph. Lambin, B. Djafari-Rouhani, A. Akjouj, L. Dobrzynski, N. Fettouhi, and J. Zemmouri
Phys. Rev. E 65, 056608 – Published 2 May 2002
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Abstract

The propagation of acoustic waves in a two-dimensional composite medium constituted of a square array of parallel copper cylinders in air is investigated both theoretically and experimentally. The band structure is calculated with the plane wave expansion (PWE) method by imposing the condition of elastic rigidity to the solid inclusions. The PWE results are then compared to the transmission coefficients computed with the finite difference time domain (FDTD) method for finite thickness composite samples. In the low frequency regime, the band structure calculations agree with the FDTD results indicating that the assumption of infinitely rigid inclusion retains the validity of the PWE results to this frequency domain. These calculations predict that this composite material possesses a large absolute forbidden band in the domain of the audible frequencies. The FDTD spectra reveal also that hollow and filled cylinders produce very similar sound transmission suggesting the possibility of realizing light, effective sonic insulators. Experimental measurements show that the transmission through an array of hollow Cu cylinders drops to noise level throughout frequency interval in good agreement with the calculated forbidden band.

  • Received 30 November 2001

DOI:https://doi.org/10.1103/PhysRevE.65.056608

©2002 American Physical Society

Authors & Affiliations

J. O. Vasseur1,*, P. A. Deymier2, A. Khelif3, Ph. Lambin3, B. Djafari-Rouhani1, A. Akjouj1, L. Dobrzynski1, N. Fettouhi4, and J. Zemmouri4

  • 1Laboratoire de Dynamique et Structures des Matériaux Moléculaires, UPRESA CNRS 8024, UFR de Physique, Université de Lille I, 59655 Villeneuve d’Ascq Cédex, France
  • 2Department of Materials Science and Engineering, University of Arizona, Tucson, Arizona 85721
  • 3Laboratoire de Physique du Solide, Département de Physique, Facultés Notre-Dame de la Paix, 5000 Namur, Belgium
  • 4Laboratoire de Physique des Lasers, Atomes et Molécules, Centre d’Etudes et de Recherches Lasers et Applications, UMR CNRS 8523, UFR de Physique, Université de Lille I, 59655 Villeneuve d’Ascq Cédex, France

  • *Corresponding author. Email address: jerome.vasseur@univ-lille1.fr

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Vol. 65, Iss. 5 — May 2002

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