Topology optimization of an acoustic metamaterial with negative bulk modulus using local resonance

Abstract During the past decade, materials that display novel properties in the acoustic realm, so-called acoustic metamaterials, have attracted much attention, since these properties can provide promising opportunities to design new acoustic devices that cannot be made with natural materials. Although acoustic metamaterials that exhibit negative mass density or negative bulk modulus, and double-negative acoustic metamaterials, have been obtained experimentally by trial and error, our aim is to develop a topology optimization method for the direct design of acoustic metamaterials, based on the concept of local resonant mechanisms, which ensures that the lattice constant is orders of magnitude functionally smaller than the corresponding sonic wavelength, and avoids unwanted effects of Bragg scattering mechanisms. This paper proposes a level set-based topology optimization method for the structural design of acoustic metamaterials that achieve an extremely negative bulk modulus at certain prescribed frequencies. Level set-based topology optimization methods can directly provide clear boundaries in optimal configurations that avoid the presence of grayscales. The optimization problem is formulated for a two-dimensional wave propagation problem, with the objective being to minimize the effective bulk modulus at chosen target frequencies. An effective medium description based on S-parameters is introduced to describe the acoustic metamaterial. Finite element method (FEM) is used to solve the Helmholtz equation for acoustic waves, sensitivities are obtained with the adjoint variable method (AVM), and a reaction-diffusion equation is used to update the level set function. Several numerical examples with prescribed target frequencies and different initial shapes are provided to demonstrate that the proposed method can provide clear, optimized structures for the design of negative bulk modulus acoustic metamaterials.

[1]  P. Sheng,et al.  Introduction to Wave Scattering, Localization and Mesoscopic Phenomena. Second edition , 1995 .

[2]  David R. Smith,et al.  Electromagnetic parameter retrieval from inhomogeneous metamaterials. , 2005, Physical review. E, Statistical, nonlinear, and soft matter physics.

[3]  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.

[4]  Masataka Yoshimura,et al.  Topology design of multi-material soundproof structures including poroelastic media to minimize sound pressure levels , 2009 .

[5]  Takayuki Yamada,et al.  A topology optimization method based on the level set method for the design of negative permeability dielectric metamaterials , 2012 .

[6]  Jin Au Kong,et al.  Robust method to retrieve the constitutive effective parameters of metamaterials. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[7]  James K. Guest,et al.  Topology optimization with multiple phase projection , 2009 .

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

[9]  Jakob Søndergaard Jensen,et al.  Low-frequency band gaps in chains with attached non-linear oscillators , 2007 .

[10]  Stewart,et al.  Extremely low frequency plasmons in metallic mesostructures. , 1996, Physical review letters.

[11]  M. Wang,et al.  Piecewise constant level set method for structural topology optimization , 2009 .

[12]  M. Bendsøe Optimal shape design as a material distribution problem , 1989 .

[13]  Ole Sigmund,et al.  Design of photonic bandgap fibers by topology optimization , 2010 .

[14]  Takayuki Yamada,et al.  A topology optimization method based on the level set method incorporating a fictitious interface energy , 2010 .

[15]  O. Sigmund Morphology-based black and white filters for topology optimization , 2007 .

[16]  Jakob S. Jensen,et al.  Acoustic design by topology optimization , 2008 .

[17]  N. Fang,et al.  Ultrasonic metamaterials with negative modulus , 2006, Nature materials.

[18]  Willie J Padilla,et al.  Composite medium with simultaneously negative permeability and permittivity , 2000, Physical review letters.

[19]  R. Martínez-Sala,et al.  SOUND ATTENUATION BY A TWO-DIMENSIONAL ARRAY OF RIGID CYLINDERS , 1998 .

[20]  Chunguang Xia,et al.  Broadband acoustic cloak for ultrasound waves. , 2010, Physical review letters.

[21]  D. Smith,et al.  Determination of effective permittivity and permeability of metamaterials from reflection and transmission coefficients , 2001, physics/0111203.

[22]  Yoon Young Kim,et al.  Topology optimization of muffler internal partitions for improving acoustical attenuation performance , 2009 .

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

[24]  Ole Sigmund,et al.  A topology optimization method for design of negative permeability metamaterials , 2010 .

[25]  A. Klarbring,et al.  Topology optimization of regions of Darcy and Stokes flow , 2007 .

[26]  Ole Sigmund,et al.  Systematic Design of Metamaterials by Topology Optimization , 2009 .

[27]  N. K. Batra,et al.  Modelling and simulation of acoustic wave propagation in locally resonant sonic materials. , 2004, Ultrasonics.

[28]  N. Fang,et al.  Focusing ultrasound with an acoustic metamaterial network. , 2009, Physical review letters.

[29]  T. E. Bruns,et al.  Topology optimization of non-linear elastic structures and compliant mechanisms , 2001 .

[30]  Gengkai Hu,et al.  Analytic model of elastic metamaterials with local resonances , 2009 .

[31]  J. Willis,et al.  On cloaking for elasticity and physical equations with a transformation invariant form , 2006 .

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

[33]  C. M. de Blok,et al.  Full Characterization of Linear Acoustic Networks Based on N-Ports and S Parameters , 1992 .

[34]  Sébastien Guenneau,et al.  Split-ring resonators and localized modes , 2004 .

[35]  Z. Sipus,et al.  Waveguide miniaturization using uniaxial negative permeability metamaterial , 2005, IEEE Transactions on Antennas and Propagation.

[36]  G. Allaire,et al.  Structural optimization using sensitivity analysis and a level-set method , 2004 .

[37]  M. Bendsøe,et al.  Generating optimal topologies in structural design using a homogenization method , 1988 .

[38]  Ole Sigmund,et al.  Systematic design of phononic band–gap materials and structures by topology optimization , 2003, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[39]  Xiaoming Wang,et al.  A level set method for structural topology optimization , 2003 .

[40]  E. E. Narimanov,et al.  The left hand of brightness: past, present and future of negative index materials , 2006, Nature materials.

[41]  Ole Sigmund,et al.  On the Design of Compliant Mechanisms Using Topology Optimization , 1997 .

[42]  Xiang Zhang,et al.  Method for retrieving effective properties of locally resonant acoustic metamaterials , 2007 .

[43]  Roderic S. Lakes,et al.  Composites with Inclusions of Negative Bulk Modulus: Extreme Damping and Negative Poisson’s Ratio , 2005 .

[44]  David R. Smith,et al.  Metamaterial Electromagnetic Cloak at Microwave Frequencies , 2006, Science.

[45]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

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

[47]  Vladimir M. Shalaev,et al.  Superlens based on metal-dielectric composites , 2005 .

[48]  J. Pendry,et al.  Magnetism from conductors and enhanced nonlinear phenomena , 1999 .