Willis elasticity from microcontinuum field theories: Asymptotics, microstructure-property relationships, and cloaking
arXiv:2310.08463 · doi:10.1016/j.wavemoti.2023.103206
Abstract
Willis elasticity is an effective medium theory for linearly elastic composites that incorporates an unusual coupling between stress and velocity, as well as between momentum and strain. Interest in the theory peaked following the discovery that its formulation is invariant under curvilinear changes of coordinates and that, consequently, it can be used to inverse-design ``invisibility'' cloaks for elastodynamics. That said, the microstructure-property relationships in Willis elasticity are poorly understood and, in particular, the mechanics that underlie the coupling are largely unknown. Thus, no such cloaks were constructed. Here, we put forward the idea that Willis elasticity is a particular microcontinuum field theory where the (generalized) micro-displacements have been eliminated in favor of the macroscopic displacement field as if by Schur completion. The field theory is special in that it features an inertial coupling between the micro- and macro-displacements that, upon completion, re-emerges as the coupling term in Willis elasticity. Concretely, we analyze an asymptotic regime where mechanical lattices exhibit a kinematic enrichment with a strong (leading-order) inertial coupling. We provide, in closed-form, the resulting microstructure-property relationships. As an application, and in light of the gained insights, we design an ``invisibility'' cloak resolved into Willis-elastic mechanical lattices.
7 figures
References in corpus (5)
- New metamaterials with macroscopic behavior outside that of continuum elastodynamics
- Employing pre-stress to generate finite cloaks for antiplane elastic waves
- Effective Willis constitutive equations for periodically stratified anisotropic elastic media
- Polar metamaterials: A new outlook on resonance for cloaking applications
- Microtwist elasticity: A continuum approach to zero modes and topological polarization in Kagome lattices