Theory of Strains in Auxetic Materials

This paper is dedicated to Prof. Jacques Friedel, an inspirational scientist and a great man. His excellence and clear vision led to significant advances in theoretical physics, which spilled into material science and technological applications. His fundamental theoretical work on commonplace materials has become classic. We can think of no better tribute to Friedel than to apply a fundamental analysis in his spirit to a peculiar class of materials—auxetic materials. Auxetic materials, or negative-Poisson’-ratio materials, are important technologically and fascinating theoretically. When loaded by external stresses, their internal strains are governed by correlated motion of internal structural degrees of freedom. The modelling of such materials is mainly based on ordered structures, despite the existence of auxetic behaviour in disordered structures and the advantage in manufacturing disordered structures for most applications. We describe here a first-principles expression for strains in disordered such materials, based on insight from a family of ‘isoauxetic’ structures. These are structures, consisting of internal structural elements, which we name ‘auxetons’, whose inter-element forces can be computed from statics alone. Iso-auxetic structures make it possible not only to identify the mechanisms that give rise to auxeticity, but also to write down the explicit dependence of the strain rate on the local structure, which is valid to all auxetic materials. It is argued that stresses give rise to strains via two mechanisms: auxeton rotations and auxeton expansion/contraction. The former depends on the stress via a local fabric tensor, which we R. Blumenfeld (!) ESE and ISP, Imperial College London, London SW7 2AZ, UK e-mail: [email protected] R. Blumenfeld · S.F. Edwards Cavendish Laboratory, Cambridge University, Cambridge CB3 0HE, UK define explicitly for 2D systems. The latter depends on the stress via an expansion tensor. Whether a material exhibits auxetic behaviour or not depends on the interplay between these two fields. This description has two major advantages: it applies to any auxeton-based system, however disordered, and it goes beyond conventional elasticity theory, providing an explicit expression for general auxetic strains and outlining the relevant equations.