2006
DOI: 10.1103/physrevb.73.064301
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Flexural vibration band gaps in Euler-Bernoulli beams with locally resonant structures with two degrees of freedom

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Cited by 206 publications
(114 citation statements)
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“…Remarkably, in periodic triangular lattices, even with a single material and building block, local resonances can be exploited to generate bandgaps, providing a foundation for the design of a new class of systems to manipulate the propagation of elastic waves. Furthermore, our results also demonstrate that, in order to attenuate the propagation of elastic waves through localized resonances, it is not necessary to embed additional resonating components 23,24,[34][35][36][37][38][39][40][41][42] within the beam lattices. Such singlebuilding-block and single-material system with locally resonant bandgap has been previously realized in onedimensional setup only 43 .…”
mentioning
confidence: 92%
“…Remarkably, in periodic triangular lattices, even with a single material and building block, local resonances can be exploited to generate bandgaps, providing a foundation for the design of a new class of systems to manipulate the propagation of elastic waves. Furthermore, our results also demonstrate that, in order to attenuate the propagation of elastic waves through localized resonances, it is not necessary to embed additional resonating components 23,24,[34][35][36][37][38][39][40][41][42] within the beam lattices. Such singlebuilding-block and single-material system with locally resonant bandgap has been previously realized in onedimensional setup only 43 .…”
mentioning
confidence: 92%
“…[5,[7][8][9][10][11][12][13][14][15][16][17][18]. Elastodynamics of finite or infinite periodic 1D rod or beam structures has been studied in [6,[19][20][21]. Comparisons between Floquet theory ( [1]) based unit cell analysis of a band structure and the vibration response analysis of the corresponding finite periodic structure, are presented in [22] for one-dimensional diatomic chains of uncoupled spheres and in [14] for 1D rod structures, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…In all these examples, the careful microscale periodic architecture of multiscale engineered material systems leads to an interesting or beneficial effective dynamic behavior on the macroscale. Besides pronounced acoustic band gaps [15,16], this design paradigm has resulted in negative effective dynamic stiffness [17] and mass density [18,19] and combinations of both [20]. Here negative stiffness and negative mass density refer to the effective dynamic properties: An elastic system containing only positive-stiffness elements can demonstrate negative effective dynamic quantities near resonance.…”
Section: Introductionmentioning
confidence: 99%