2018
DOI: 10.1016/j.compositesb.2018.07.012
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Band gap behaviour of optimal one-dimensional composite structures with an additive manufactured stiffener

Abstract: In this work, the banded behaviour of composite one-dimensional structures with an additive manufactured stiffener is examined. A finite element method is used to calculate the stiffness, mass and damping matrices, and periodic structure theory is used to obtain the wave propagation of one-dimensional structures.A multi-disciplinary design optimisation scheme is developed to achieve optimal banded behaviour and structural characteristics of the structures under investigation. Having acquired the optimal soluti… Show more

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Cited by 27 publications
(19 citation statements)
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“…Non strut-based AM BG lattices can be seen in the work of Elmadih et al [18] and Abueidda et al [8]; in both these cases, BG structures were obtained using lattices based on triply periodic minimal surface (TPMS) equations. Non strut-based AM BG lattices can also be seen in the ceramic lattice work of Kruisová et al [33] and Ampatzidis et al [17].…”
Section: Introductionmentioning
confidence: 80%
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“…Non strut-based AM BG lattices can be seen in the work of Elmadih et al [18] and Abueidda et al [8]; in both these cases, BG structures were obtained using lattices based on triply periodic minimal surface (TPMS) equations. Non strut-based AM BG lattices can also be seen in the ceramic lattice work of Kruisová et al [33] and Ampatzidis et al [17].…”
Section: Introductionmentioning
confidence: 80%
“…The concept of BGs emerged from solid-state physics, with recent use in electronic systems [1,2,3], photonics [4,5,6,7] and phononic structures [8,9,10,11,12,13]. BGs generally result from Bragg scattering, in which transmitted and reflected waves within a periodic medium undergo destructive interference [14,15,16,17,18,19]. The BG frequencies depend on the geometry and size of the repeating lattice unit cell [20].…”
Section: Introductionmentioning
confidence: 99%
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“…In addition to the unusual mechanical and physical properties, architected materials have been designed and optimized for novel elastodynamic wave phenomena. One example of such architected materials is phononic metamaterial, which consists of periodically topological structures and materials dispersions and has the ability to manipulate the propagation of mechanical waves [17][18][19][20][21][22][23][24][25][26][27][28][29]. The periodic structures of phononic crystals produce omnidirectional band gaps-ranges of frequencies where elastic waves cannot propagate.…”
Section: Introductionmentioning
confidence: 99%
“…Due to periodicity, the wave propagation characteristics of a periodic structure are governed by the dynamics of a single unit cell (smallest repetitive substructure). Hence one can intentionally design the material and geometric parameters, as well as the boundary conditions of the unit cell to tailor or artificially create band gaps [ 20 , 21 ]. These artificial periodic structures are often referred to as phononic crystals [ 5 , 22 ].…”
Section: Introductionmentioning
confidence: 99%