Global gradient estimate for a divergence problem and its application to the homogenization of a magnetic suspension

preprint2022arXivOpen access

Abstract

This paper generalizes the results obtained by the authors in \cite{dangHomogenizationNondiluteSuspension2021} concerning the homogenization of a non-dilute suspension of magnetic particles in a viscous flow. More specifically, in this paper, a restrictive assumption on the coefficients of the coupled equation, made in \cite{dangHomogenizationNondiluteSuspension2021}, that significantly narrowed the applicability of the homogenization results obtained, is relaxed and a new regularity of the solution of the fine-scale problem is proven. In particular, we obtain a global L∞L^{\infty}-bound for the gradient of the solution of the scalar equation −div[a(x/ε)∇φε(x)]=f(x)-\mathrm{div} \left[ \mathbf{a} \left( x/\varepsilon \right)\nabla φ^{\varepsilon}(x) \right] = f(x), uniform with respect to microstructure scale parameter ε≪1\varepsilon\ll 1 in a small interval (0,ε0)(0,\varepsilon_0), where the coefficient a\mathbf{a} is only \emph{piecewise} Hölder continuous. Thenceforth, this regularity is used in the derivation of the effective response of the given suspension discussed in \cite{dangHomogenizationNondiluteSuspension2021}.

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