2021
DOI: 10.1177/10812865211059220
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In-plane dynamic buckling of duoskelion beam-like structures: discrete modeling and numerical results

Abstract: In this contribution, a previously introduced discrete model for studying the statics of duoskelion beam-like structures is extended to dynamics. The results of numerical simulations performed using such an extended model are reported to discuss the in-plane dynamic buckling of duoskelion structures under different loading and kinematic boundary conditions. The core instrument of the analysis is a discrete beam element, which, in addition to flexure, also accounts for extension and shearing deformations. Worki… Show more

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Cited by 17 publications
(11 citation statements)
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“…We can formulate Hooke’s law to define the stress tensor as a linear combination of the volumetric and deviatoric strain tensors: where K is the bulk modulus and G is the shear modulus. From Equation ( 1 ), it is possible then to recognize the two contributions to the stress, namely the hydrostatic: and shear or deviatoric part: This formulation can be generalized by using mechanical micromorphic [ 47 , 48 , 49 , 50 , 51 , 52 , 53 , 54 , 55 , 56 ], micropolar [ 57 , 58 , 59 , 60 ], higher-order [ 61 , 62 , 63 , 64 , 65 , 66 , 67 , 68 , 69 , 70 ], or peridynamic [ 71 , 72 , 73 , 74 ] models. As an opening move, the stiffnesses can be evaluated starting with the knowledge of the engineering parameters, Young’s modulus Y , and Poisson’s ratio as follows: since they are more str...…”
Section: Methodsmentioning
confidence: 99%
“…We can formulate Hooke’s law to define the stress tensor as a linear combination of the volumetric and deviatoric strain tensors: where K is the bulk modulus and G is the shear modulus. From Equation ( 1 ), it is possible then to recognize the two contributions to the stress, namely the hydrostatic: and shear or deviatoric part: This formulation can be generalized by using mechanical micromorphic [ 47 , 48 , 49 , 50 , 51 , 52 , 53 , 54 , 55 , 56 ], micropolar [ 57 , 58 , 59 , 60 ], higher-order [ 61 , 62 , 63 , 64 , 65 , 66 , 67 , 68 , 69 , 70 ], or peridynamic [ 71 , 72 , 73 , 74 ] models. As an opening move, the stiffnesses can be evaluated starting with the knowledge of the engineering parameters, Young’s modulus Y , and Poisson’s ratio as follows: since they are more str...…”
Section: Methodsmentioning
confidence: 99%
“…Micromorphic materials [171][172][173][174][175][176][177]; 3. Granular materials and metamaterials based on such concept [178][179][180][181][182][183]; 4. Fiber-reinforced materials [184][185][186]; 5.…”
Section: Current Times: Deep Investigations In Generalized Continuamentioning
confidence: 99%
“…Many efforts for the definition of meso-models for the analysis of these lattice structures have been presented: high-order beam formulations can be found in the previous studies [40][41][42]. In Turco et al [43] and Eugster [44], the wave propagation in lattice structures is investigated by means of meso-models composed by beams. Some examples presented in this contribution show as the proposed formulation is a very useful tool for analyzing the non-linear and post-buckling behavior of this kind of structures.…”
Section: Introductionmentioning
confidence: 99%