Dispersive homogenized models and coefficient formulas for waves in general periodic media

preprint2014arXivOpen access

Abstract

We analyze a homogenization limit for the linear wave equation of second order. The spatial operator is assumed to be of divergence form with an oscillatory coefficient matrix aεa^\varepsilon that is periodic with characteristic length scale ε\varepsilon; no spatial symmetry properties are imposed. Classical homogenization theory allows to describe solutions uεu^\varepsilon well by a non-dispersive wave equation on fixed time intervals (0,T)(0,T). Instead, when larger time intervals are considered, dispersive effects are observed. In this contribution we present a well-posed weakly dispersive equation with homogeneous coefficients such that its solutions wεw^\varepsilon describe uεu^\varepsilon well on time intervals (0,Tε−2)(0,T\varepsilon^{-2}). More precisely, we provide a norm and uniform error estimates of the form ∥uε(t)−wε(t)∥≤Cε\| u^\varepsilon(t) - w^\varepsilon(t) \| \le C\varepsilon for t∈(0,Tε−2)t\in (0,T\varepsilon^{-2}). They are accompanied by computable formulas for all coefficients in the effective models. We additionally provide an ε\varepsilon-independent equation of third order that describes dispersion along rays and we present numerical examples.

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