Computational design of locally resonant acoustic metamaterials

Abstract The so-called Locally Resonant Acoustic Metamaterials (LRAM) are considered for the design of specifically engineered devices capable of stopping waves from propagating in certain frequency regions (bandgaps), this making them applicable for acoustic insulation purposes. This fact has inspired the design of a new kind of lightweight acoustic insulation panels with the ability to attenuate noise sources in the low frequency range (below 5000 Hz) without requiring thick pieces of very dense materials. A design procedure based on different computational mechanics tools, namely, (1) a multiscale homogenization framework, (2) model order reduction strategies and (3) topological optimization procedures, is proposed. It aims at attenuating sound waves through the panel for a target set of resonance frequencies as well as maximizing the associated bandgaps. The resulting design’s performance is later studied by introducing viscoelastic properties in the coating phase, in order to both analyse their effects on the overall design and account for more realistic behaviour. The study displays the emerging field of Computational Material Design (CMD) as a computational mechanics area with enormous potential for the design of metamaterial-based industrial acoustic parts.

[1]  M. Nouh,et al.  Metadamping and energy dissipation enhancement via hybrid phononic resonators , 2018 .

[2]  M. Ruzzene,et al.  Dynamics of Phononic Materials and Structures: Historical Origins, Recent Progress, and Future Outlook , 2014 .

[3]  P. Blanco,et al.  Variational Foundations and Generalized Unified Theory of RVE-Based Multiscale Models , 2016 .

[4]  Ping Sheng,et al.  Acoustic metamaterial panels for sound attenuation in the 50–1000 Hz regime , 2010 .

[5]  James M. Manimala,et al.  Microstructural design studies for locally dissipative acoustic metamaterials , 2014 .

[6]  Massimo Ruzzene,et al.  Broadband plate-type acoustic metamaterial for low-frequency sound attenuation , 2012 .

[7]  V. Kouznetsova,et al.  Visco-elastic effects on wave dispersion in three-phase acoustic metamaterials , 2016 .

[8]  Jihong Wen,et al.  Sound insulation property of membrane-type acoustic metamaterials carrying different masses at adjacent cells , 2013 .

[9]  Takayuki Yamada,et al.  Topology optimization for locally resonant sonic materials , 2014 .

[10]  M. Hussein Reduced Bloch mode expansion for periodic media band structure calculations , 2008, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[11]  Mahmoud I. Hussein,et al.  Metadamping: An emergent phenomenon in dissipative metamaterials , 2013 .

[12]  Emilio P. Calius,et al.  Negative mass sound shielding structures: Early results , 2009 .

[13]  J. Oliver,et al.  A computational multiscale homogenization framework accounting for inertial effects: application to acoustic metamaterials modelling , 2018 .

[14]  Ping Sheng,et al.  Measurements of sound transmission through panels of locally resonant materials between impedance tubes , 2005 .

[15]  V. Kouznetsova,et al.  A semi-analytical approach towards plane wave analysis of local resonance metamaterials using a multiscale enriched continuum description , 2017 .

[16]  V. Kouznetsova,et al.  The attenuation performance of locally resonant acoustic metamaterials based on generalised viscoelastic modelling , 2017 .

[17]  Wim Desmet,et al.  A lightweight vibro-acoustic metamaterial demonstrator: Numerical and experimental investigation , 2016 .

[18]  P. Sheng,et al.  Locally resonant sonic materials , 2000, Science.

[19]  M. Geers,et al.  Homogenization of locally resonant acoustic metamaterials towards an emergent enriched continuum , 2016, Computational Mechanics.

[20]  Michael J. Frazier,et al.  Viscous-to-viscoelastic transition in phononic crystal and metamaterial band structures. , 2015, The Journal of the Acoustical Society of America.