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An optimal error estimate in stochastic homogenization of discrete elliptic equations

机译:离散椭圆方程随机均质化的最优误差估计

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This paper is the companion article to [Ann. Probab. 39 (2011) 779-856]. We consider a discrete elliptic equation on the d-dimensional lattice ?~d with random coefficients A of the simplest type: They are identically distributed and independent from edge to edge. On scales large w.r.t. the lattice spacing (i.e., unity), the solution operator is known to behave like the solution operator of a (continuous) elliptic equation with constant deterministic coefficients. This symmetric "homogenized" matrix A_hom = a_(hom)Id is characterized by ξ???A_(hom)ξ = ?(ξ + ??)???A(ξ + ??)? for any direction ξ ∈ ?~d, where the random field ? (the "corrector") is the unique solution of ??*???A(ξ + ??) = 0 in ?~d such that ?(0) = 0, ?? is stationary and ???? = 0, ??? denoting the ensemble average (or expectation). In order to approximate the homogenized coefficients A_(hom), the corrector problem is usually solved in a box Q_L = [?L, L)~d of size 2L with periodic boundary conditions, and the space averaged energy on Q_L defines an approximation A_L of A_(hom). Although the statistics is modified (independence is replaced by periodic correlations) and the ensemble average is replaced by a space average, the approximation A_L converges almost surely to A_(hom) as L ↑ ∞. In this paper, we give estimates on both errors. To be more precise, we do not consider periodic boundary conditions on a box of size 2L, but replace the elliptic operator by T~(?1) ? ?~????A? with (typically) T ~ L~2, as standard in the homogenization literature. We then replace the ensemble average by a space average on Q_L, and estimate the overall error on the homogenized coefficients in terms of L and T.
机译:本文是[Ann。 Probab。 39(2011)779-856]。我们考虑在d维晶格上的离散椭圆方程,其中具有最简单类型的随机系数A:它们是相同分布的,并且对于边到边都是独立的。规模大w.r.t.在已知晶格间距(即单位)的情况下,求解算子的行为类似于具有恒定确定性系数的(连续)椭圆方程的求解算子。该对称的“均质”矩阵A_hom = a_(hom)Id的特征在于ξ∑A_(hom)ξ=α(ξ+ ∑)∑A(ξ+ ∑)∑。对于任意方向ξ∈?〜d,随机场? (“校正器”)是Δ* d中Δ** A(ξ+Δθ)= 0的唯一解,使得Δ(0)= 0,Δω是固定的,???? = 0,???表示整体平均值(或期望值)。为了近似均匀化的系数A_(hom),通常在周期为边界条件的大小为2L的方框Q_L = [?L,L)〜d中解决校正器问题,并且Q_L上的空间平均能量定义为近似值A_L的A_(hom)。尽管修改了统计量(用周期相关性代替了独立性),并且用空间平均值代替了集成平均数,但是近似值A_L几乎可以确定地收敛为A_(hom)为L↑∞。在本文中,我们对这两个误差进行了估算。更准确地说,我们不考虑大小为2L的盒子上的周期边界条件,而是用T〜(?1)代替椭圆算子。 ?〜???? (通常)T〜L〜2作为均质文献的标准。然后,我们用Q_L上的空间平均值替换系综平均值,并根据L和T估计均匀系数的整体误差。

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