2020
DOI: 10.48550/arxiv.2007.10828
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Analytical and numerical study of a modified cell problem for the numerical homogenization of multiscale random fields

Abstract: A central question in numerical homogenization of partial differential equations with multiscale coefficients is the accurate computation of effective quantities, such as the homogenized coefficients. Computing homogenized coefficients requires solving local corrector problems followed by upscaling relevant local data. The most naive way of computing homogenized coefficients is by solving a local elliptic problem, which is known to suffer from the so-called resonance error dominating all other errors inherent … Show more

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Cited by 2 publications
(4 citation statements)
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“…We finally state the main result of this section, which is the sub-optimal moment bound on the time dependent flux q r (T, •) for 1 2 ≤ r ≤ √ T .…”
Section: Y) (349)mentioning
confidence: 98%
See 1 more Smart Citation
“…We finally state the main result of this section, which is the sub-optimal moment bound on the time dependent flux q r (T, •) for 1 2 ≤ r ≤ √ T .…”
Section: Y) (349)mentioning
confidence: 98%
“…(ii) Second, the semigroup u e has been used more recently in [1] for approximating φ e via exponential regularization, that is we replace the corrector equation (1.1) by u e (T ) − ∇ • a(∇φ e,T,R + e) = 0 in Q R , φ e,T,R ≡ 0 on ∂Q R , for R ≫ 1 and T ≫ 1. Optimal estimates on u e are used to control the bias (or the systematic error).…”
Section: Introductionmentioning
confidence: 99%
“…Without loss of generality, we may assume that R ≥ 2r * (0). Indeed, otherwise, we deduce from the 1 8 -Lipschitz property of r * (x) in form of…”
Section: Proof Of Lemma 4: Pointwise Estimates On the Dual Problemmentioning
confidence: 99%
“…We refer to [16] for an analysis via a semigroup approach. (ii) Second, the semigroup u e has been used more recently in [1] for approximating φ e via exponential regularization, that is we replace the corrector equation (1.1) by u e (T ) − ∇ • a(∇φ e,T ,R + e) = 0 in Q R , φ e,T ,R ≡ 0 o n ∂Q R ,…”
Section: Introductionmentioning
confidence: 99%