2018
DOI: 10.1098/rspa.2018.0312
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Disarrangements and instabilities in augmented one-dimensional hyperelasticity

Abstract: In the present work, the overall nonlinear elastic behavior of a 1D multi-modular structure incorporating possible imperfections at the discrete (micro-scale) level, is derived with respect to both tensile and compressive applied loads. The model is built up through the repetition of n units, each one comprising two rigid rods having equal lengths, linked by means of pointwise constraints capable to elastically limit motions in terms of relative translations (sliders) and rotations (hinges). The mechanical res… Show more

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Cited by 11 publications
(13 citation statements)
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“…11 (see e.g. Deseri and Owen, 2003;Deseri and Owen, 2010;Deseri and Owen, 2012;Deseri and Owen, 2015;Deseri and Owen, 2019;Palumbo et al, 2018 ), as discussed in details in Appendix C .…”
Section: Declaration Of Competing Interestmentioning
confidence: 99%
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“…11 (see e.g. Deseri and Owen, 2003;Deseri and Owen, 2010;Deseri and Owen, 2012;Deseri and Owen, 2015;Deseri and Owen, 2019;Palumbo et al, 2018 ), as discussed in details in Appendix C .…”
Section: Declaration Of Competing Interestmentioning
confidence: 99%
“…Structured Deformations (see e.g. Deseri and Owen, 2003;Deseri and Owen, 2010;Deseri and Owen, 2012;Deseri and Owen, 2015;Deseri and Owen, 2019;Palumbo et al, 2018 ) is a multiscale geometric framework that permits to account for both conformational changes and remodelling arising at the submacroscopic level. Such a framework does allow for envisioning three full configurations for the membrane.…”
Section: Conformational Changes Remodelling and Associated Energeticsmentioning
confidence: 99%
“…Now, it is natural to explore what happens if the number of discrete elements becomes infinite while their size tends to zero. This can be effectively achieved by adopting the so-called first-order SD theory, which gives a unique way to pass from discrete to continuum without loss of information about displacements and their spatial gradients, allowing one to interpret the classical (smooth) macroscopic motion of a body as the projection of non-classical (piecewise-smooth) deformations occurring at the sub-macroscopic scale [15,19,2630]. We will call these media—resulting from an initially discrete structure through a limit procedure and preserving internal discontinuities (disarrangements)— structured continua .…”
Section: From Discrete To Continuum Via Structured Deformations: Kinematics Of Structured Continuamentioning
confidence: 99%
“…Motivated by the vast variety of inputs and challenges posed by the current research in materials and by the opportunity to unveil some possible logics underlying the response of metamaterials, in this work, we exploit a simple— ad hoc designed—mechanism of mutual sliding between rigid tesserae, interconnected via pre-tensed hyperelastic cables, to obtain uniaxial and biaxial structures capable of offering simultaneously various uncommon mechanical responses. Multi-scale kinematics with local disarrangements [15], tensile buckling [16], instability-induced auxetic properties [17,18] related to chiral deformation modes arising from initially achiral (bulky and geometrically symmetrical) configurations, non-symmetrical responses to compressive and tensile loads as well as deck-of-cards deformation modes producing macroscopic shear [19] are in fact all replicated in the paradigmatic system studied here. In particular, we start from the case of a uniaxial multi-element macro-system comprising an arbitrary number of sub-units, so obtaining tunable critical buckling loads and stiffness if macroscopically stretched under tensile forces, reproducing instead overall shear as a sort of complementary version of the kinematics exhibited by Timoshenko beams if forces are applied orthogonally to the axis of the uniaxial system.…”
Section: Introductionmentioning
confidence: 97%
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