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Abstracts (International Journals and Books)

[35]   K. Itatani, I. J. Davies, H. Kuwano, and M. Aizawa, “Sinterability of magnesium silicon nitride powder with yttrium oxide addition coated using the homogeneous precipitation method”, J. Maters. Sci., 37(4) pp. 737-744 (2002).

Abstract: Properties of MgSiN2 powder with 0-4 mass% Y2O3 addition coated using the homogeneous precipitation method and their resulting hot-pressed compacts (31 MPa/1550 oC/N2/90 min) were investigated. Mg/Si ratios for the MgSiN2 compacts with Y2O3 addition were close to unity for all cases whilst the pure MgSiN2 ceramic contained 3.0 mass% of oxygen and that of the MgSiN2 ceramic with 1 mass% of Y2O3 addition contained 1.2 mass%. Relative densities of the pure MgSiN2 ceramics with and without Y2O3 additions were ~99% apart for the compact with 4 mass% Y2O3 addition (~98%). Vickers hardness of the pure MgSiN2 compact hot-pressed at 1550 oC for 90 min was 19.7 GPa whilst the thermal conductivity was as low as 20 W·m-1·K-1 and attributed to the presence of a secondary phase (Y2Si3O3N4) that surrounded the MgSiN2 grains together with the small average grain size.

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[34]   S. Tanaka, K. Itatani, H. Uchida, M. Aizawa, I. Okada, I. J. Davies, H. Suemasu, and A. Nozue, “The effect of rare-earth oxide addition on the hot-pressing of magnesium silicon nitride”, J. Eur. Ceram. Soc., 22(5) pp. 777-783 (2002).

Abstract: The effect of rare-earth oxide addition (1-5 mass% of Ln2O3 addition; Ln=Y, La, Nd, Sm, Gd, Dy, Er, and Yb) on the properties of hot-pressed (1550 oC, 90 min, 31 MPa) magnesium silicon nitride (MgSiN2) has been investigated. The role of rare-earth oxide addition on the relative density was classified as follows: (i) positive effect (Y2O3, La2O3, and Yb2O3 additions), (ii) no appreciable effect (Nd2O3 and Er2O3 additions), and (iii) negative effect (Sm2O3, Gd2O3, and Dy2O3 additions). The average grain size (0.3-0.9 mm) for hot-pressed MgSiN2 compacts with rare-earth oxide addition was smaller compared to that of the pure MgSiN2 compact (0.95 mm). The average Vickers hardness of the MgSiN2 ceramic with 1 mass% of Y2O3 addition showed the highest value (21.5 GPa) amongst the MgSiN2 ceramics with rare-earth oxide addition. The thermal conductivity of the MgSiN2 ceramics was maximum for the case of 1 mass% of Yb2O3 addition (26.6 W·m-1·K-1) and is believed to be the highest value so far reported for MgSiN2. Overall, it was concluded that the relative density and Vickers hardness were best enhanced through the use of Y2O3 addition whereas the addition of Yb2O3 was most suitable for enhancing the thermal conductivity.

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[33]   K. Itatani, F. Takahashi, M. Aizawa, I. Okada, I. J. Davies, H. Suemasu, and A. Nozue, “Densification and microstructural developments during the sintering of aluminium silicon carbide”, J. Maters. Sci., 37(2) pp. 335-342 (2002).

Abstract: Densification and microstructural developments during the sintering of aluminium silicon carbide (Al4SiC4) were examined. Two types of Al4SiC4 powders were prepared by the solid-state reactions between: (i) Al, Si, and C at 1600 oC for 10 h (designated as Al4SiC4(SSR)), and (ii) chemically-vapour deposited ultrafine Al 4C 3 and SiC powders at 1500 oC for 4 h (Al4SiC4(CVD/SSR)). The specific surface areas of the Al4SiC4(SSR) and Al4SiC4(CVD/SSR) powders were 2.7 and 15.5 m2·g-1, respectively. Relative densities of the pressureless-sintered Al4SiC4(SSR) and Al4SiC4(CVD/SSR) compacts were as low as 60~70% for firing temperatures between 1700 oC and 2000 oC. The relative densities of Al4SiC4(SSR) and Al4SiC4(CVD/SSR) compacts could be enhanced using the hot-pressing technique with that of the Al4SiC4(SSR) compact hot-pressed at 1900 oC for 3 h being 97.0% whereas that of the Al4SiC4(CVD/SSR) compact hot-pressed at 1900 oC for 1 h attained 99.0%. The former microstructure was composed of plate-like grains of width 10~30 mm and thickness ~10 mm whilst the latter microstructure was comprised of equiaxed grains with a typical diameter of 10 mm. Densification of the Al4SiC4(CVD/SSR) compacts appeared to be promoted compared to the Al4SiC4(SSR) compact and this was attributed to the higher surface area, reduced agglomeration of the starting primary particles, and more homogeneous chemical composition.

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[32]   I. J. Davies, T. Ogasawara, and T. Ishikawa, “Scanning electron microscopy study of failure in glass-sealed SiC/SiC-based composite (NUSK-CMC) creep tested at 1100 and 1200 oC in air”, Adv. Composite Maters., 10(4) pp. 357-367 (2001).

Abstract: A scanning electron microscopy investigation was carried out for glass-sealed 3D woven SiC/SiC-based composite that had failed following creep testing at 1100 and 1200 oC in air. It was shown that most specimens failed due to oxygen ingression into the composite that initiated at the specimen corner. The main path for oxygen movement with specimens was found to be along z fibre bundles. A simple analysis of the glass evaporation rate showed higher evaporation rates to always exist at the specimen corners and this could help to explain initiation of long-term creep failure.

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[31]   I. J. Davies, T. Ogasawara, and T. Ishikawa, “Fibre/matrix interface shear strength estimated from fibre pullout length data for Tyranno® Si-Zr-C-O fibre composites with different SiC-based matrices and interfaces”, J. Maters. Sci. Letts., 20(23) pp. 2127-2130 (2001).

Abstract: The present work has indicated that reasonable values for the fibre/matrix interface shear strength, τ, for Tyranno® Si-Zr-C-O fiber composites with different silicon carbide-based matrices and interfaces may be qualitatively estimated using only fiber pullout length data together with a previously determined correction factor. The resulting values of τ were slightly below those noted for Tyranno® Si-Ti-C-O fiber composites but generally within the range of 2–22 MPa noted by previous researchers.

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