Multi-resonator metamaterials as multi-band metastructures

被引:29
|
作者
Gorshkov, Vyacheslav [1 ,2 ]
Sareh, Pooya [3 ]
Navadeh, Navid [4 ]
Tereshchuk, Vladimir [1 ]
Fallah, Arash S. [4 ,5 ,6 ]
机构
[1] Natl Tech Univ Ukraine, Dept Phys, Igor Sikorsky Kiev Polytech Inst, Bldg 7,37 Peremogy Ave, UA-03056 Kiev 56, Ukraine
[2] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
[3] Univ Liverpool, Sch Engn, Dept Mech Mat & Aerosp, Creat Design Engn Lab Cdel, Brownlow Hill, Liverpool L69 3GH, Merseyside, England
[4] Imperial Coll London, Dept Aeronaut, City & Guilds Bldg,South Kensington Campus, London SW7 2AZ, England
[5] Oslo Metropolitan Univ, Dept Machinery Elect & Chem, Pilestredet 35, N-0166 Oslo, Norway
[6] ZHAWZurich Univ Appl Sci, ICP Inst Computat Phys, Wildbachstr 21, CH-8401 Winterthur, Switzerland
关键词
Multi-resonator; Phononic metamaterial; Acoustic mode; Optic mode; Bandgap; Dispersion surface;
D O I
10.1016/j.matdes.2021.109522
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Introducing multi-resonator microstructure into phononic metamaterials provides more flexibility in bandgap manipulation. In this work, 3D-acoustic metamaterials of the body- and face-centered cubic lattice systems encompassing nodal isotropic multivibrators are investigated. Our main results are: (1) the number of bandgaps equals the number, n, of internal masses as each bandgap is a result of the classical analog of the quantum level-repulsion mechanism between internal and external oscillations, and (2) the upper boundary frequencies, omega(2i)(upper), i = 1, 2, ..., n, of the gaps formed coincide with eigen-frequencies, omega(2)(int;i) not equal 0, of the isolated multivibrator, omega(upper2;i) = omega(2)(int; i), and the lower boundary frequencies, omega(2)(lower2,i), are in good agreement with estimations as omega(2)(lower;i)approximate to(omega) over cap (2)(int;i) (omega(2)(lower;i) < <(omega)over cap>(2)(int;i)), where (omega) over cap (2)(int;i) represent the eigen-frequencies of the multivibrator when its external shell is motionless. The morphologies of the set of dispersion surfaces, omega(2)(m)(k), m = 1, 2, ..., 6, in the corresponding passbands are similar to each other and to that of the set of dispersion surfaces, omega(2)(ext; m)(k), obtained through the exclusion of internal masses. Thus, the problem of analyzing the acoustic properties of the complicated system is reduced to the study of two simple sets {omega(2)(int; i)} and {(omega) over cap (2)(int;i)}, along with {omega(2)(ext; m)(k)}, the morphology of which depends only on the type of lattice symmetry. This splitting renders controlled phononic bandgaps formation in homogeneous multi-resonator metamaterials feasible. (C) 2021 The Author(s). Published by Elsevier Ltd.
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页数:13
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