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7] M. E. Glicksman, “Analysis of 3-D network structures,” Philosophical Magazine, 85 (2005) 3–31.  D. J. Rowenhorst, A. C. Lewis, and G. Spanos, “Three-dimensional analysis of grain topology and interface curvature in a β-titanium alloy,” Acta Materialia, 58 (2010) 5511–5519.  Y. Suwa, Y. Saito, and H. Onodera, “Parallel computer simulation of threedimensional grain growth using the multi-phase-ﬁeld model,” Materials Transactions, 49 (2008) 704–709.  M. Elsey, S. Esedo¯glu, and P. Smereka, “Large-scale simulation of normal grain growth via diﬀusion-generated motion,” Proceedings of the Royal Society A: Mathematical, Physical and Engineering Science, 467 (2011) 381–401.
A) (b) (c) (d) (e) SiC Fe-20Cr Fig. 0 MPa is analyzed. Simulated result of the stress under load 2 MPa is showed in Fig. 2. From Fig. 0 MPa, the stress mainly distributes in SiC networks. From Fig. 82 MPa, respectively. The stress distribution of SiC reinforcement has relatively different in different directions. Especially, the stress goes up tremendously in near the interface boundary, the max stress appears in the interfacial boundary of the Fe–20Cr and SiC, or edge or the joints of the SiC network.
W Xing, X. M Cao, W. P. Hu, et al. “Interfacial reactions in 3D–SiC network reinforced Cu–matrix composites prepared by squeeze casting,” Materials Letters,59(2005),1563–1566. J Zhao, N. Li, L. Z Zhao, X. L. Zhang, “Numerical Simulations of Compression Properties of SiC/Al Co-continuous Composites”, IFIP AICT ,347(2011), 480–485.  M. Pavese, M. Valle, C. Badini, “Effect of porosity of cordierite performs on microstructure and mechanical strength of co–continuous ceramic composites,” Journal of the European Ceramic Society, 27 (2007), 131–141.