Abstract:We revisit the periodic homogenization of Dirichlet problems for the Laplace operator in perforated domains, and establish a unified proof that works for different regimes of hole-cell ratios, that is the ratio between the scaling factor of the holes and that of the periodic cells. The approach is then made quantitative and it yields correctors and error estimates for vanishing holecell ratios. For positive volume fraction of holes, the approach is just the standard oscillating test function method; for vanish… Show more
“…Similar results are expected to hold in dimension d = 2 but would require a different treatment, as e.g. in [6,41]. The hole ηT is assumed to be an non-empty open subset strictly included in the unit cell for any η ≤ 1 (it does not touch the boundary):…”
Section: 3mentioning
confidence: 69%
“…The asymptotic behaviors of the tensors X k * , M k are obtained by following the methodology of [6,41,34], which relies on several technical results stated in this part.…”
Section: 3mentioning
confidence: 99%
“…This matter is to be adressed in a future work through a more accurate analysis of the rate of convergence of the coefficients X 2k * and X 2k+1 * in the asymptotic (5.12) and (5.13). To date, let us note that Jing obtained recently X 0 * = F/η d−2 + O(1) in the scalar case (proof of the Lemma 5.1 in [41]) by using layer potential techniques.…”
We derive high order homogenized models for the incompressible Stokes system in a cubic domain filled with periodic obstacles. These models have the potential to unify the three classical limit problems (namely the "unchanged" Stokes system, the Brinkman model, and the Darcy's law) corresponding to various asymptotic regimes of the ratio η ≡ aε/ε between the radius aε of the holes and the size ε of the periodic cell. What is more, a novel, rather surprising feature of our higher order effective equations is the occurrence of odd order differential operators when the obstacles are not symmetric. Our derivation relies on the method of two-scale power series expansions and on the existence of a "criminal" ansatz, which allows to reconstruct the oscillating velocity and pressure (uε, pε) as a linear combination of the derivatives of their formal average (u * ε , p * ε ) weighted by suitable corrector tensors. The formal average (u * ε , p * ε ) is itself the solution to a formal, infinite order homogenized equation, whose truncation at any finite order is in general ill-posed. Inspired by the variational truncation method of [53,27], we derive, for any K ∈ N, a well-posed model of order 2K + 2 which yields approximations of the original solutions with an error of order O(ε K+3 ) in the L 2 norm. Furthermore, the error improves up to the order O(ε 2K+4 ) if a slight modification of this model remains well-posed. Finally, we find asymptotics of all homogenized tensors in the low volume fraction limit η → 0 and in dimension d ≥ 3. This allows us to obtain that our effective equations converge coefficient-wise to either of the Brinkman or Darcy regimes which arise when η is respectively equivalent, or greater than the critical scaling η crit ∼ ε 2/(d−2) .
“…Similar results are expected to hold in dimension d = 2 but would require a different treatment, as e.g. in [6,41]. The hole ηT is assumed to be an non-empty open subset strictly included in the unit cell for any η ≤ 1 (it does not touch the boundary):…”
Section: 3mentioning
confidence: 69%
“…The asymptotic behaviors of the tensors X k * , M k are obtained by following the methodology of [6,41,34], which relies on several technical results stated in this part.…”
Section: 3mentioning
confidence: 99%
“…This matter is to be adressed in a future work through a more accurate analysis of the rate of convergence of the coefficients X 2k * and X 2k+1 * in the asymptotic (5.12) and (5.13). To date, let us note that Jing obtained recently X 0 * = F/η d−2 + O(1) in the scalar case (proof of the Lemma 5.1 in [41]) by using layer potential techniques.…”
We derive high order homogenized models for the incompressible Stokes system in a cubic domain filled with periodic obstacles. These models have the potential to unify the three classical limit problems (namely the "unchanged" Stokes system, the Brinkman model, and the Darcy's law) corresponding to various asymptotic regimes of the ratio η ≡ aε/ε between the radius aε of the holes and the size ε of the periodic cell. What is more, a novel, rather surprising feature of our higher order effective equations is the occurrence of odd order differential operators when the obstacles are not symmetric. Our derivation relies on the method of two-scale power series expansions and on the existence of a "criminal" ansatz, which allows to reconstruct the oscillating velocity and pressure (uε, pε) as a linear combination of the derivatives of their formal average (u * ε , p * ε ) weighted by suitable corrector tensors. The formal average (u * ε , p * ε ) is itself the solution to a formal, infinite order homogenized equation, whose truncation at any finite order is in general ill-posed. Inspired by the variational truncation method of [53,27], we derive, for any K ∈ N, a well-posed model of order 2K + 2 which yields approximations of the original solutions with an error of order O(ε K+3 ) in the L 2 norm. Furthermore, the error improves up to the order O(ε 2K+4 ) if a slight modification of this model remains well-posed. Finally, we find asymptotics of all homogenized tensors in the low volume fraction limit η → 0 and in dimension d ≥ 3. This allows us to obtain that our effective equations converge coefficient-wise to either of the Brinkman or Darcy regimes which arise when η is respectively equivalent, or greater than the critical scaling η crit ∼ ε 2/(d−2) .
“…In this paper, we focus on the case with zero Neumann data at the boundary of the holes, and investigate the continuous transition of the effective models with respect to the relative smallness of the holes, and we establish quantitative convergence results for homogenization when the holes are dilute. The proofs are based on a careful study of the rescaled cell-problems using layer potential techniques, a method started in [25,26,27] for the case of Dirichlet data in the holes, and exhibit the effectiveness of this approach. Before we refocus on the problem (1.1), let us mention that homogenizations in perforated domains and in similar geometric settings have gained many attentions recently with new convergence rates and uniform regularity [36,38,39,35,40,30] following the framework of [10,11,31,29], derivations in the non-periodic settings [23,22,21,20], derivation of higher order models [17,16,18] and so on.…”
Section: Introductionmentioning
confidence: 99%
“…σ ε is the bounding constant of a version of Poincaré inequality for H 1 functions in B ε with zero value in B ηε ; see e.g. [2,25]. Note that η cr,2 ∼ ε 2 d−2 for d ≥ 3 and η cr,2 ∼ exp(− C ε 2 ) for d = 2.…”
We revisit the homogenization problem for the Poisson equation in periodically perforated domains with zero Neumann data at the boundary of the holes and prescribed Dirichlet data at the outer boundary. It is known that, if the periodicity of the holes goes to zero but their volume fraction remains fixed and positive, the limit problem is a Dirichlet boundary value problem posed in the domain without the holes, and the effective diffusion coefficients are non-trivially modified; if that volume fraction goes to zero instead, i.e. the holes are dilute, the effective operator remains the Laplacian (that is, unmodified). Our main results contain the study of a "continuity" in those effective models with respect to the volume fraction of the holes and some new convergence rates for homogenization in the dilute setting. Our method explores the classical two-scale expansion ansatz and relies on asymptotic analysis of the rescaled cell problems using layer potential theory.
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