Disarrangements and instabilities in 1D hyperelasticity

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 response of the structure is analyzed by varying the number n of the elemental moduli, as well as in the limit case of infinite number of infinitesimal constituents, in light of the theory of (first order) Structured Deformations (SDs), that interprets the deformation of any continuum body as the projection, at the macroscopic scale, of geometrical changes occurring at the level of its sub-macroscopic elements. In this way, a wide family of nonlinear elastic behaviors is generated by tuning internal microstructural parameters, the tensile buckling and the classical Euler Elastica under compressive loads resulting as special cases in the so-called continuum limit, say when n tends to 1. Finally, by plotting the results in terms of first Piola-Kirchhoff stress versus macroscopic stretch, it is for the first time demonstrated that such SDs-based 1D models can be helpfully used to generalize some standard hyperelastic behaviors by additionally taking into account instability phenomena and concealed defects.

[1]  M. Fraldi,et al.  Nonlinear elasticity and buckling in the simplest soft-strut tensegrity paradigm , 2018, International Journal of Non-Linear Mechanics.

[2]  M. Fraldi,et al.  Cells competition in tumor growth poroelasticity , 2018 .

[3]  D. Owen Elasticity with Gradient-Disarrangements: A Multiscale Perspective for Strain-Gradient Theories of Elasticity and of Plasticity , 2017 .

[4]  C. Spadaccio,et al.  Stress-shielding, growth and remodeling of pulmonary artery reinforced with copolymer scaffold and transposed into aortic position , 2016, Biomechanics and modeling in mechanobiology.

[5]  D. Owen,et al.  Submacroscopic Disarrangements Induce a Unique, Additive and Universal Decomposition of Continuum Fluxes , 2016 .

[6]  D. Owen,et al.  Stable disarrangement phases arising from expansion/contraction or from simple shearing of a model granular medium , 2015 .

[7]  Ivo Caliò,et al.  Tensile and compressive buckling of columns with shear deformation singularities , 2015 .

[8]  D. Owen,et al.  Stable disarrangement phases of elastic aggregates: a setting for the emergence of no-tension materials with non-linear response in compression , 2014 .

[9]  D. Ingber,et al.  Tensegrity, cellular biophysics, and the mechanics of living systems , 2014, Reports on progress in physics. Physical Society.

[10]  M. Fraldi,et al.  Analytical solutions for n-phase Functionally Graded Material Cylinders under de Saint Venant load conditions: Homogenization and effects of Poisson ratios on the overall stiffness , 2013 .

[11]  D. Bigoni Nonlinear Solid Mechanics: Bifurcation Theory and Material Instability , 2012 .

[12]  Eugenio Ruocco,et al.  An analytical model for the buckling of plates under mixed boundary conditions , 2012 .

[13]  D. Misseroni,et al.  Structures buckling under tensile dead load , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[14]  D. Owen,et al.  Submacroscopically Stable Equilibria of Elastic Bodies Undergoing Disarrangements and Dissipation , 2010 .

[15]  K. Bertoldi,et al.  Negative Poisson's Ratio Behavior Induced by an Elastic Instability , 2010, Advanced materials.

[16]  S. Cowin,et al.  Inhomogeneous elastostatic problem solutions constructed from stress-associated homogeneous solutions , 2004 .

[17]  D. Owen,et al.  Toward a Field Theory for Elastic Bodies Undergoing Disarrangements , 2003 .

[18]  D. Ingber Tensegrity I. Cell structure and hierarchical systems biology , 2003, Journal of Cell Science.

[19]  Vlado A. Lubarda,et al.  On the mechanics of solids with a growing mass , 2002 .

[20]  D. Owen,et al.  Invertible structured deformations and the geometry of multiple slip in single crystals , 2002 .

[21]  Heng Xiao,et al.  Hencky's elasticity model and linear stress-strain relations in isotropic finite hyperelasticity , 2002 .

[22]  K. Evans,et al.  Auxetic Materials : Functional Materials and Structures from Lateral Thinking! , 2000 .

[23]  I. Müller Two instructive instabilities in non-linear elasticity: Biaxially loaded membrane, and rubber balloons , 1996 .

[24]  S. Nemat-Nasser,et al.  Micromechanics: Overall Properties of Heterogeneous Materials , 1993 .

[25]  G. Piero,et al.  Structured deformations of continua , 1993 .

[26]  R. Lakes Foam Structures with a Negative Poisson's Ratio , 1987, Science.

[27]  Lallit Anand,et al.  On H. Hencky’s Approximate Strain-Energy Function for Moderate Deformations , 1979 .

[28]  S. Timoshenko,et al.  Theory of Elasticity (3rd ed.) , 1970 .

[29]  R. Hill,et al.  On constitutive inequalities for simple materials—I , 1968 .

[30]  A. Ibrahimbegovic Nonlinear Solid Mechanics , 2009 .

[31]  Dimitrije Stamenović,et al.  Cytoskeletal Mechanics: Models of cytoskeletal mechanics based on tensegrity , 2006 .

[32]  D. Owen Elasticity with Disarrangements , 2004 .

[33]  D. Owen Structured deformations and the refinements of balance laws induced by microslip , 1998 .