Mechanical structure-property relationship of aerogels

被引:144
作者
Ma, HS
Roberts, AP
Prévost, JH
Jullien, R
Scherer, GW
机构
[1] Princeton Univ, Dept Chem Engn, Princeton, NJ 08544 USA
[2] Univ Queensland, Ctr Microscopy & Microanal, St Lucia, Qld 4072, Australia
[3] Princeton Univ, Dept Civil & Environm Engn, Princeton, NJ 08544 USA
[4] Univ Montpellier 2, CNRS, UA 1119, Lab Sci Mat Vitreux, F-34095 Montpellier 5, France
关键词
D O I
10.1016/S0022-3093(00)00288-X
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
The elastic moduli (E) of high-porosity materials (such as aerogels) exhibit power-law scaling with their relative densities (rho), E proportional to rho (m)(,) where 3 less than or equal to m less than or equal to 4, but the physics responsible for this behavior is not well-understood, Computer models of aerogels were generated by diffusion-limited cluster-cluster aggregation (DLCA) algorithms, and their linear elastic properties were examined by the finite element method (FEM), assuming that the stiffness of each interparticle bond can be represented by a beam element. The simulation yields m approximate to 3.6 for perfectly connected structures, contradicting the consensus that the dangling mass on the gel gives rise to the exponent. The results suggest that the high exponent is largely because of the reduction in the connectivity of the material with decreasing density. The open-cell foam model, which predicts m = 2, is valid only when the connectivity remains unchanged upon variation of the density. The mechanical structure-property relationship in the gel can be described by the 'blob-and-link' model. The bonds (links) between the fractal clusters (blobs) are more sparsely distributed than those inside the clusters, and therefore the strain energy is localized at the cluster boundaries during deformation. This model is consistent with the experimental evidence. (C) 2000 Elsevier Science B.V. All rights reserved.
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页码:127 / 141
页数:15
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