2022
DOI: 10.1016/j.mechrescom.2022.103889
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Bandgap merging with double-negative metabeam

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Cited by 11 publications
(3 citation statements)
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“…However, the bandgaps are very narrower and limit its applications. Therefore, graded frequency LRs [25][26][27], nonlinear elements [28][29][30], and bandgaps merging [31][32][33][34] and tuneable technologies [35][36][37][38][39] are considered in metastructures to suppress vibration in wider, adjustable and adaptive bandgaps. Lv et al [40] designed a tuneable elastic metamaterial beam using rotatable coupled dual beam LRs, which can continuously tune the bandgap and transmission properties of the metamaterial beam by changing the moment of inertia of the resonators in a wide frequency range.…”
Section: Introductionmentioning
confidence: 99%
“…However, the bandgaps are very narrower and limit its applications. Therefore, graded frequency LRs [25][26][27], nonlinear elements [28][29][30], and bandgaps merging [31][32][33][34] and tuneable technologies [35][36][37][38][39] are considered in metastructures to suppress vibration in wider, adjustable and adaptive bandgaps. Lv et al [40] designed a tuneable elastic metamaterial beam using rotatable coupled dual beam LRs, which can continuously tune the bandgap and transmission properties of the metamaterial beam by changing the moment of inertia of the resonators in a wide frequency range.…”
Section: Introductionmentioning
confidence: 99%
“…This enables novel properties for vibration attenuation [6][7][8][9], focusing and rerouting [10,11], non-reciprocity [12], or wave amplification for energy harvesting [13][14][15]. On the topic of vibration attenuation, numerous works have shown the potential and the advantages of using local resonators [16][17][18][19][20][21]. These structures generally consist of a main waveguide, that can be 1D (a beam) 2D (a plate) or 3D (a bulk solid), inside of which are placed local resonators.…”
Section: Introductionmentioning
confidence: 99%
“…𝑑 2 e βˆ’π‘˜π‘₯ + 𝑑 3 e +π‘–π‘˜π‘₯ + 𝑑 4 e +π‘˜π‘₯ (4 16). where the wave number for flexural wave mode can be defined by π‘˜ = √ area of the uniform beam section.…”
mentioning
confidence: 99%