An Improved Analytical Model for the Elastic Constants of Auxetic and Conventional Hexagonal Honeycombs

Cellular solids, in particular hexagonal honeycombs have been the subject of numerous studies in the last decades in view of their extensive use in many applications. In particular, there have been various studies aimed at expressing the mechanical properties of honeycombs in terms of the geometrical parameters used to describe the structure of such honeycombs. Despite improvements over the first established model, finite element simulations performed in this work on honeycombs having ribs with a realistic thickness-to-length ratio suggest that the mechanical properties for such systems differ from those predicted by current models, sometimes to a very significant extent. In view of this, we analyse in detail the deformed structures in an attempt to gain insight into how and the extent to which the shape of the ligaments, in particular its thickness and mode of connection affects deformation in conventional and re-entrant hexagonal honeycombs. Based on these observations, we propose a modified version of the previous analytical models that take into consideration the finite thickness of the ligaments.

[1]  K. Evans,et al.  Microscopic examination of the microstructure and deformation of conventional and auxetic foams , 1997 .

[2]  Robert Almgren,et al.  An isotropic three-dimensional structure with Poisson's ratio =−1 , 1985 .

[3]  K. E. EVANS,et al.  Molecular network design , 1991, Nature.

[4]  Fabrizio Scarpa,et al.  Shape memory behaviour in auxetic foams: mechanical properties , 2010 .

[5]  Kenneth E. Evans,et al.  Auxetic two-dimensional polymer networks. An example of tailoring geometry for specific mechanical properties , 1995 .

[6]  Ruben Gatt,et al.  On the properties of auxetic meta‐tetrachiral structures , 2008 .

[7]  Roderic S. Lakes,et al.  Deformation mechanisms in negative Poisson's ratio materials: structural aspects , 1991 .

[8]  O. Sigmund,et al.  Design and fabrication of compliant micromechanisms and structures with negative Poisson's ratio , 1996, Proceedings of Ninth International Workshop on Micro Electromechanical Systems.

[9]  Kenneth E. Evans,et al.  Mass transport properties of auxetic (negative Poisson's ratio) foams , 2007 .

[10]  Hiro Tanaka,et al.  In-plane mechanical behaviors of 2D repetitive frameworks with four-coordinate flexible joints and elbowed beam members , 2009 .

[11]  M. Ashby,et al.  The mechanics of two-dimensional cellular materials , 1982, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[12]  Fabrizio Scarpa,et al.  Transverse elastic shear of auxetic multi re-entrant honeycombs , 2009 .

[13]  Massimo Ruzzene,et al.  Auxetic compliant flexible PU foams: static and dynamic properties , 2005 .

[14]  Ruben Gatt,et al.  On the potential of connected stars as auxetic systems , 2005 .

[15]  Farhan Gandhi,et al.  Zero Poisson’s Ratio Cellular Honeycombs for Flex Skins Undergoing One-Dimensional Morphing , 2010 .

[16]  Fabrizio Scarpa,et al.  Stiffness and energy dissipation in polyurethane auxetic foams , 2008 .

[17]  I. Burgess,et al.  A theoretical approach to the deformation of honeycomb based composite materials , 1979 .

[18]  Philip J. Withers,et al.  In situ three-dimensional X-ray microtomography of an auxetic foam under tension , 2009 .

[19]  Kenneth E. Evans,et al.  Indentation Resilience of Conventional and Auxetic Foams , 1998 .

[20]  Kenneth E. Evans,et al.  Auxetic foams: Modelling negative Poisson's ratios , 1994 .

[21]  Kenneth E. Evans,et al.  The Mechanical Properties of Conventional and Auxetic Foams. Part I: Compression and Tension , 1999 .

[22]  Fabrizio Scarpa,et al.  A novel centresymmetric honeycomb composite structure , 2005 .

[23]  R. Lakes,et al.  Properties of a chiral honeycomb with a poisson's ratio of — 1 , 1997 .

[24]  Fabrizio Scarpa,et al.  Dynamic properties of high structural integrity auxetic open cell foam , 2004 .

[25]  Fabrizio Scarpa,et al.  Physical and thermal effects on the shape memory behaviour of auxetic open cell foams , 2010 .

[26]  Joseph N. Grima,et al.  Modelling of hexagonal honeycombs exhibiting zero Poisson's ratio , 2011 .

[27]  Ruben Gatt,et al.  A Novel Process for the Manufacture of Auxetic Foams and for Their re‐Conversion to Conventional Form , 2009 .

[28]  Fabrizio Scarpa,et al.  Tensile fatigue of conventional and negative Poisson’s ratio open cell PU foams , 2009 .

[29]  K. Evans,et al.  Modelling the mechanical properties of an auxetic molecular network , 1994 .

[30]  Fabrizio Scarpa,et al.  Mechanical behaviour of conventional and negative Poisson’s ratio thermoplastic polyurethane foams under compressive cyclic loading , 2007 .

[31]  Ole Sigmund,et al.  On the design of 1–3 piezocomposites using topology optimization , 1998 .

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

[33]  K. Evans,et al.  Models for the elastic deformation of honeycombs , 1996 .

[34]  Fabrizio Scarpa,et al.  Theoretical characteristics of the vibration of sandwich plates with in-plane negative poisson's ratio values , 2000 .

[35]  Ruben Gatt,et al.  Elastic constants of 3-, 4- and 6-connected chiral and anti-chiral honeycombs subject to uniaxial in-plane loading , 2010 .

[36]  K. Evans,et al.  Strain dependent densification during indentation in auxetic foams , 1999 .

[37]  Joseph N. Grima,et al.  A novel mechanism for generating auxetic behaviour in reticulated foams: missing rib foam model , 2000 .