Abstract
In this work, a general boundary element procedure is proposed to obtain the effective elastic tensor of solids containing randomly distributed micro-cavities in terms of its primary elastic properties. The average-field theory and a special boundary element formulation are combined to carry out a statistical analysis on the numerical results obtained for a Representative Volume Element (RVE). The two-dimensional isotropic material is simulated as a homogeneous matrix containing cylindrical holes. In the proposed implementation each hole boundary is modeled with a single boundary element. The average variables of the micro-field are evaluated using boundary-only data, which leads to a formulation particularly suitable for Boundary Element Methods. Expressions for effective elastic properties as a function of the micro-fields for both isotropic and transversally isotropic hypothesis are derived. Finally, the methodology is illustrated with some application examples and the results are compared with analytical and experimental results.
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Acknowledgements
The first author wishes to express his gratitude to CNPq (Brazil) for the financial support and to Prof. Adrián P. Cisilino (National University of Mar del Plata, Argentina) for useful discussions. The authors are also grateful to Prof. V. Mantič for his comments on the original manuscript. This work was partially financed by PROSUL 490185/2005-3 and CAPES/SECYP 048/03 projects.
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Appendix
Appendix
The shape functions used by the hole elements are presented below.
-
3-noded element (as proposed by Henry and Banerjee [4]):
$$ \begin{aligned} M_1 \left(\theta \right)=&\frac{1}{3}+\frac{2}{3}\hbox{cos}\, \theta \\ M_2 \left(\theta \right)=&\frac{1}{3}+\frac{\sqrt{3}}{3}\hbox{sin}\, \theta -\frac{1}{3}\hbox{cos}\, \theta \\ M_3 \left(\theta \right)=&\frac{1}{3}-\frac{\sqrt{3}}{3}\hbox{sin}\, \theta -\frac{1}{3}\hbox{cos}\, \theta \end{aligned} $$ -
4-noded element:
$$ \begin{aligned} M_1 \left(\theta \right)=&\frac{\left(1+\hbox{cos}\, \theta \right)}{2}\hbox{cos}\, \theta \\ M_2 \left(\theta \right)=&\frac{1}{2}+\frac{1}{2}\hbox{sin}\, \theta -\frac{1}{2}\hbox{cos}^{2}\theta \\ M_3 \left(\theta \right)=&\frac{\left(-1+\hbox{cos}\, \theta \right)}{2}\hbox{cos}\, \theta \\ M_4 \left(\theta \right)=&\frac{1}{2}-\frac{1}{2}\hbox{sin}\, \theta -\frac{1}{2}\hbox{cos}^{2}\theta \end{aligned} $$ -
5-noded element:
$$ \begin{aligned} M_1 \left(\theta \right)=&\frac{\hbox{cos}^{2}\theta +\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta -\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta -\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)}{\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)-\hbox{cos} \left(\frac{\pi}{5} \right)+\hbox{cos} \left(\frac{2\pi}{5} \right)-1}\\ M_2 \left(\theta \right)=&\frac{\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta \hbox{sin}\, \theta -\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{sin}\, \theta +\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{sin}\, \theta -\hbox{cos}\, \theta \hbox{sin}\, \theta}{\Uppsi}\\ &+\frac{\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos}^{2}\theta -\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta +\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta -\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)}{\Uppsi}\\ M_3 \left(\theta \right)=&\frac{\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{sin}\, \theta +\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{sin}\, \theta -\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta \hbox{sin}\, \theta -\hbox{cos}\, \theta \hbox{sin}\, \theta}{\Upsigma}\\ &+\frac{\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos}^{2}\theta -\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta -\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta +\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)}{\Upsigma}\\ M_4 \left(\theta \right)=&\frac{-\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{sin}\, \theta -\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{sin}\, \theta +\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta \hbox{sin}\, \theta +\hbox{cos}\, \theta \hbox{sin}\, \theta}{\Upsigma}\\ &+\frac{\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos}^{2}\theta -\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta -\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta +\hbox{sin} \left(\frac{\pi}{5} \right)\hbox{cos} \left(\frac{2\pi}{5} \right)}{\Upsigma}\\ M_5 \left(\theta \right)=&\frac{-\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{sin}\, \theta -\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{sin}\, \theta \hbox{cos}\, \theta +\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{sin}\, \theta +\hbox{cos}\, \theta \hbox{sin}\, \theta}{\Uppsi}\\ &+\frac{\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos}^{2}\theta +\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)\hbox{cos}\, \theta -\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos}\, \theta -\hbox{sin} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)}{\Uppsi} \end{aligned} $$where
$$ \begin{aligned} \Uppsi =&2\hbox{sin} \left(\frac{2\pi}{5} \right)\left[ \hbox{cos}^{2}\left(\frac{2\pi}{5} \right)-\hbox{cos} \left(\frac{2\pi}{5} \right)+\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)-\hbox{cos} \left(\frac{\pi}{5} \right) \right]\\ \Upsigma =&4\hbox{sin} \left(\frac{\pi}{5} \right)\left[ \hbox{cos}^{2}\left(\frac{\pi}{5} \right)+\hbox{cos} \left(\frac{2\pi}{5} \right)+\hbox{cos} \left(\frac{2\pi}{5} \right)\hbox{cos} \left(\frac{\pi}{5} \right)+\hbox{cos} \left(\frac{\pi}{5} \right) \right] \end{aligned} $$ -
6-noded element:
$$ \begin{aligned} M_1 \left(\theta \right)=&-\frac{1}{6}-\frac{1}{6}\hbox{cos}\, \theta +\frac{2}{3}\hbox{cos}^{2}\theta +\frac{2}{3}\hbox{cos}^{3}\theta\\ M_2 \left(\theta \right)=&\frac{\sqrt{3}}{6}\hbox{sin}\, \theta +\frac{\sqrt{3}}{3}\hbox{sin}\, \theta \hbox{cos}\, \theta -\frac{1}{3}\hbox{cos}^{2}\theta -\frac{2}{3}\hbox{cos}^{3}\theta +\frac{2}{3}\hbox{cos}\, \theta +\frac{1}{3}\\ M_3 \left(\theta \right)=&\frac{\sqrt{3}}{6}\hbox{sin}\, \theta -\frac{\sqrt{3}}{3}\hbox{sin}\, \theta \hbox{cos}\, \theta -\frac{2}{3}\hbox{cos}\, \theta -\frac{1}{3}\hbox{cos}^{2}\theta +\frac{2}{3}\hbox{cos}^{3}\theta +\frac{1}{3}\\ M_4 \left(\theta \right)=&-\frac{1}{6}+\frac{1}{6}\hbox{cos}\, \theta +\frac{2}{3}\hbox{cos}^{2}\theta -\frac{2}{3}\hbox{cos}^{3}\theta\\ M_5 \left(\theta \right)=&-\frac{\sqrt{3}}{6}\hbox{sin}\, \theta +\frac{\sqrt{3}}{3}\hbox{sin}\, \theta \hbox{cos}\, \theta -\frac{2}{3}\hbox{cos}\, \theta -\frac{1}{3}\hbox{cos}^{2}\theta +\frac{2}{3}\hbox{cos}^{3}\theta +\frac{1}{3} \\ M_6 \left(\theta \right)=&-\frac{\sqrt{3}}{6}\hbox{sin}\, \theta -\frac{\sqrt{3}}{3}\hbox{sin}\, \theta \hbox{cos}\, \theta +\frac{2}{3}\hbox{cos}\, \theta -\frac{1}{3}\hbox{cos}^{2}\theta -\frac{2}{3}\hbox{cos}^{3}\theta +\frac{1}{3} \end{aligned} $$
The shape functions for 4, 5, and 6-noded elements were proposed in [13]. It is important to point out that all the functions describe exactly rigid body movements of the holes.
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Buroni, F.C., Marczak, R.J. Effective properties of materials with random micro-cavities using special boundary elements. J Mater Sci 43, 3510–3521 (2008). https://doi.org/10.1007/s10853-008-2479-3
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DOI: https://doi.org/10.1007/s10853-008-2479-3