Free and forced wave propagation in beam lattice metamaterials with viscoelastic resonators

TL;DR

This paper develops a spectral design framework for beam lattice metamaterials with viscoelastic resonators, enabling control over wave propagation and band gap creation through a novel integral-differential equation approach.

Contribution

It introduces a dynamic formulation for dispersion analysis in beam lattice metamaterials with viscoelastic resonators, incorporating a Boltzmann superposition integral and Prony series approximation.

Findings

Dispersion spectra are characterized by complex branches.

Band gaps can be engineered through microstructural parameters.

Taylor series approximations provide insights into wave behavior.

Abstract

Beam lattice materials are characterized by a periodic microstructure realizing a geometrically regular pattern of elementary cells. In these microstructured materials, the dispersion properties governing the free dynamic propagation of elastic waves can be studied by formulating parametric lagrangian models and applying the Floquet-Bloch theory. Within this framework, governing the wave propagation by means of spectral design techniques and/or energy dissipation mechanisms is a major issue of theoretical and applied interest. Specifically, the wave propagation can be inhibited by purposely designing the microstructural parameters to open band gaps in the material spectrum at target center frequencies. Based on these motivations, a general dynamic formulation for determining the dispersion properties of beam lattice metamaterials, equipped with local resonators is presented. The mechanism of local resonance is realized by tuning periodic auxiliary masses, viscoelastically coupled with the beam lattice microstructure. As peculiar aspect, the viscoelastic coupling is derived by a mechanical formulation based on the Boltzmann superposition integral, whose kernel is approximated by a Prony series. Consequently, the free propagation of damped waves is governed by a linear homogeneous system of integral-differential equations of motion. Therefore, differential equations of motion with frequency-dependent coefficients are obtained by applying the bilateral Laplace transform. The corresponding complex-valued branches characterizing the dispersion spectrum are determined and parametrically analyzed. Particularly, the spectra corresponding to Taylor series approximations of the equation coefficients are investigated.