By Eros Dimitriou, Marco Petralia

During this textual content, fabrication procedures of particle bolstered ceramic are brought, which supply an invaluable set of variables for version experimental and theoretical stories. Toughening mechanisms of particle dispersion bolstered ceramic matrix composites also are mentioned.

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Figure 4. Treatment of UHMPE fibers in the two-roll mill. 24 Petroula A. Tarantili This will allow the preparation of composites with increased filler volume fraction and consequently, better mechanical performance. This research has shown, in fact, that calendering of UHMPE fibers is a process which significantly improves their performance as reinforcement in cases of complex loading. Although no conclusive evidence has been found so far about the changes in the fiber microstructure, it was clear that calendered UHMPE fibers at 130oC give improved performance in composites especially for low filler volume fraction.

Technol. 2000, 60, 1873-1878. 46 Petroula A. -S. Europ. Polym. J. 2002, 38, 79-86. [29] Gu, H. Mater. and Design 2009, 30, 867-870. ; Ryu, S. Compos. Sci. Technol. 2008, 68, 3208-3214. [31] Mai, Y. ; Castino, F. J. Mater. Sci. 1984, 19, 1638-1655. -W. J. Mater. Sci. 1991, 26, 4702-4720. [33] Varelidis, P. ; Papakostopoulos, D. , Pandazis, C. ; Papaspyridis, C. D. Compos. Part A 2000, 31, 549-558. ; Brisson, J. Polym. Comp. 2007, 28, 278-286. [35] Allred, R. ; Street, K. ; Martinez, R. J. Proceeding of the 24th National SAMPE Symposium, Asuza, California (1979) p.

14 shows that the impact strength of epoxy specimens reinforced with as-received Surface Modification of Ultra High Modulus Polymeric Fibers 37 aramid fibers shows a linear increase with fiber content, whereas those contained coated fibers show a constant impact strength, with resole resin giving lower strength than the novolac. This is an additional evidence that better interfacial adhesion does not contribute to improved impact characteristics. This latest statement is associated with the energy absorption by the tested material as a function of the path of crack propagation.

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