Influence of nonlinear subunits on the resonance frequency band gaps of acoustic metamaterial

Recently, a significant attention has been directed toward so called ‘acoustic metamaterials’ which have large similarity with already-known ‘electromagnetic metamaterials’ which are applied for elimination of the electromagnetic waves. The stop of electromagnetic waves is realized with the negative refractive index, negative permittivity and negative permeability. Motivated by the mathematical analogy between acoustic and electromagnetic waves, the acoustic metamaterials are introduced. It was asked the material to have negative effective mass. To obtain the negative effective mass, the artificial material, usually composite, has to be designed. The basic unit is a vibration absorber which consists of a lumped mass attached with a spring to the basic mechanical system. The purpose of the unit is to give a band gap where some frequencies of acoustic wave are stopped. We investigated the nonlinear mass-in-mass unit excited with any periodic force. Mathematical model of the motion is a system of two coupled strongly nonlinear and nonhomogeneous second-order differential equations. The solution of equations is assumed in the form of the Ateb (inverse beta) periodic function. The frequency of vibration is obtained as the function of the parameters of the excitation force. The effective mass of the system is also determined. Regions of negative effective mass are calculated. For these values the motion of the forced mass stops. It is concluded that the stop frequency gaps are much wider for the nonlinear than for the linear system. Based on the obtained parameter values, the acoustic metamaterial could be designed.

[1]  Imre J. Rudas,et al.  From the smart hands to tele-operations , 2016 .

[2]  Livija Cveticanin,et al.  Oscillator with a Sum of Noninteger-Order Nonlinearities , 2012, J. Appl. Math..

[3]  Jensen Li,et al.  Double-negative acoustic metamaterial. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[4]  Guoliang Huang,et al.  On the negative effective mass density in acoustic metamaterials , 2009 .

[5]  Exact solutions for the response of purely nonlinear oscillators: Overview , 2016 .

[6]  W. Ji-hong,et al.  Sound Absorption of Locally Resonant Sonic Materials , 2006 .

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

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

[9]  Chunyin Qiu,et al.  Metamaterial with simultaneously negative bulk modulus and mass density. , 2007, Physical review letters.

[10]  Gengkai Hu,et al.  Experimental study on negative effective mass in a 1D mass–spring system , 2008 .

[11]  C. Sun,et al.  A chiral elastic metamaterial beam for broadband vibration suppression , 2014 .

[12]  P. Pai,et al.  Acoustic metamaterial beams based on multi-frequency vibration absorbers , 2014 .

[13]  Y Y Chen,et al.  Wave propagation and absorption of sandwich beams containing interior dissipative multi‐resonators , 2017, Ultrasonics.

[14]  L. Cvetićanin A solution procedure based on the Ateb function for a two-degree-of-freedom oscillator , 2015 .

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

[16]  Bhisham Sharma,et al.  Dynamic behaviour of sandwich structure containing spring-mass resonators , 2011 .

[17]  P. Frank Pai,et al.  Metamaterial-based Broadband Elastic Wave Absorber , 2010 .

[18]  C. Sun,et al.  Optimizing the Band Gap of Effective Mass Negativity in Acoustic Metamaterials , 2012 .

[19]  R. M. Rosenberg,et al.  On Nonlinear Vibrations of Systems with Many Degrees of Freedom , 1966 .

[20]  L. Cvetićanin Pure Nonlinear Oscillator , 2014 .

[21]  G. Milton New metamaterials with macroscopic behavior outside that of continuum elastodynamics , 2007, 0706.2202.

[22]  S. A. Neild,et al.  Out-of-unison resonance in weakly nonlinear coupled oscillators , 2015, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[23]  C. Sun,et al.  Wave attenuation mechanism in an acoustic metamaterial with negative effective mass density , 2009 .

[24]  Per-Gunnar Martinsson,et al.  VIBRATIONS OF LATTICE STRUCTURES AND PHONONIC BAND GAPS , 2003 .

[25]  P. Sheng,et al.  Analytic model of phononic crystals with local resonances , 2005 .

[26]  V. Veselago The Electrodynamics of Substances with Simultaneously Negative Values of ∊ and μ , 1968 .

[27]  Meiping Sheng,et al.  Multi-flexural band gaps in an Euler–Bernoulli beam with lateral local resonators , 2016 .

[28]  Yu Song,et al.  Trapping and attenuating broadband vibroacoustic energy with hyperdamping metamaterials , 2017 .

[29]  Graeme W Milton,et al.  On modifications of Newton's second law and linear continuum elastodynamics , 2007, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[30]  Yoon Young Kim,et al.  Effective mass density based topology optimization of locally resonant acoustic metamaterials for bandgap maximization , 2016 .

[31]  P. Pai,et al.  Acoustic metamaterial plates for elastic wave absorption and structural vibration suppression , 2014 .

[32]  Xiang Zhang,et al.  Negative refractive index in chiral metamaterials. , 2009, Physical review letters.

[34]  Miodrag Zukovic,et al.  Negative effective mass in acoustic metamaterial with nonlinear mass-in-mass subsystems , 2017, Commun. Nonlinear Sci. Numer. Simul..

[35]  Liu Zhi-ming,et al.  Ultrawide Bandgap Locally Resonant Sonic Materials , 2005 .