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Statistical ensemble error bounds for homogenized microheterogeneous solids
Authors:T I Zohdi
Institution:(1) Department of Mechanical Engineering, University of California, 6195 Etcheverry Hall, Berkeley, CA 94720-1740, USA
Abstract:Typically, in order to characterize the homogenized effective macroscopic response of new materials possessing random heterogeneous microstructure, a relation between averages $
{\left\langle {\user2{ \sigma }} \right\rangle }_{\Omega } = \mathbb{E}^{*} :{\left\langle {\user2{ \epsilon }} \right\rangle }_{\Omega } 
$
is sought, where $
{\left\langle \cdot \right\rangle }_{\Omega } {\mathop = \limits^{{\text{def}}} }\tfrac{1}
{{|\Omega |}}{\int_\Omega { \cdot \,d} }\Omega ,
$
and where $\varvec{\sigma}$
and $\varvec{\epsilon}$
are the stress and strain tensor fields within a statistically representative volume element (SRVE) of volume |OHgr|. The quantity, $
\mathbb{E}^{*} ,
$
is known as the effective property, and is the elasticity tensor used in usual macroscale analyses. In order to generate homogenized responses computationally, a series of detailed boundary value representations resolving the heterogeneous microstructure, posed over the SRVErsquos domain, must be solved. This requires an enormous numerical effort that can overwhelm most computational facilities. A natural way of generating an approximation to the SRVErsquos response is by first computing the response of smaller (subrepresentative) samples, each with a different random realization of the microstructural type under investigation, and then to ensemble average the results afterwards. Compared to a direct simulation of an SRVE, testing many small samples is a computationally inexpensive process since the number of floating point operations is greatly reduced, as well as the fact that the samplesrsquo responses can be computed trivially in parallel. However, there is an inherent error in this process. Clearly the populationrsquos ensemble average is not the SRVErsquos response. However, as shown in this work, the moments on the distribution of the population can be used to generate rigorous upper and lower error bounds on the quality of the ensemble-generated response. Two-sided bounds are given on the SRVE response in terms of the ensemble average, its standard deviation and its skewness.Received: December 11, 2001
Keywords:Ensemble error bounds  homogenized properties  higher order moments
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