Pure Rutile Nano Crystalline Phase (Synthesis and Physical Properties)

2015 ◽  
Vol 3 (3) ◽  
pp. 229-232
Author(s):  
I. Kashif ◽  
H. Farouk ◽  
A. Ratep ◽  
M. Al Mahalawy
2013 ◽  
Vol 343 ◽  
pp. 286-292 ◽  
Author(s):  
M.A. Amer ◽  
T.M. Meaz ◽  
A.G. Mostafa ◽  
H.F. El-Ghazally

2020 ◽  
Author(s):  
Husniyah Aliyah Lutpi ◽  
Hasmaliza Mohamad ◽  
Tuti Katrina Abdullah

Abstract The present work aims to investigate the effects of isothermal treatment on the structural, microstructure and physical properties of Li2O-Al2O3-SiO2 glass-ceramic. Sintering temperature plays a major role in producing the desired lithium aluminosilicate (LAS) glass-ceramic crystalline phases. This work also aims to achieve a low thermal expansion coefficient β-spodumene (LiAlSi2O6) crystalline phase with improved density and lower porosity, which can be useful for the applications with thermal shock properties. The LAS glass-ceramic was fabricated by the melt-quenching technique at 1550 °C for 5 h before being isothermally sintered at an elevated temperature of 900 to 1200 °C for 30 min. The evolution of LAS glass-ceramic crystalline phases was identified using differential thermal analysis and the β-spodumene exothermic peak appeared at 999 °C. Based on the X-ray diffraction results, the complete transformation of β-spodumene from high-quartz solid solution (β-quartz) occurred at 1000 °C. However, the sintering temperature did not change the crystalline phase when sintered above 1000 °C, but the lattice parameter of the crystal structure was slightly altered. Moreover, it was observed that the LAS glass-ceramic grain size increased with temperature, whereby the smallest average grain size recorded (0.61 µm) for LAS glass-ceramic sintered at 1100 °C. Meanwhile, the fully densified LAS glass-ceramic at 1100 ° C was measured at 2.47 g/cm3 with 0.52% porosity. The isothermal treatment at elevated temperature indicated that sintering at 1100 °C provided a denser, less porous, and small average grain size which is preferred for thermal shock resistance applications.


2020 ◽  
Vol 582 ◽  
pp. 411975
Author(s):  
Ilyas Noor Bhatti ◽  
Imtiaz Noor Bhatti ◽  
Rabindra Nath Mahato ◽  
M.A.H. Ahsan

2007 ◽  
Vol 1048 ◽  
Author(s):  
Yukichi Umakoshi ◽  
Takeshi Nagase ◽  
Takashi Hosokawa

AbstractElectron irradiation induced phase transition behavior of Zr-Pd and Zr-Pt alloys was investigated focusing on phase selection in crystallization by thermal annealing and electron irradiation. Nano quasi-crystalline (QC) phase was formed by thermal crystallization in Zr66.7Pd33.3 and Zr80Pt20 alloys, while nano two-type f.c.c. super-saturated solid solutions were formed by irradiation induced crystallization at 298K. In Zr66.7Pt33.3 alloy, polycrystalline Zr5Pt3 and Zr9Pt11 phases transformed to two-type f.c.c. nano-crystalline phase through an amorphous state by crystal-to-amorphous-to-crystal (C-A-C) transition during electron irradiation. Nano-composite phase composed of f.c.c. super-saturated solid solution and residual amorphous phase was stable rather than an amorphous single phase, thermal equilibrium crystalline phase and quasi-crystalline phase under 2.0MV electron irradiation at 298K, resulting in the formation of nano-composite structure by irradiation induced amorphization and crystallization.


2014 ◽  
Vol 118 (11) ◽  
pp. 5896-5907 ◽  
Author(s):  
Takashi Tsuji ◽  
Natsuki Hosoya ◽  
Suguru Fukazawa ◽  
Rion Sugiyama ◽  
Takeshi Iwasa ◽  
...  

2016 ◽  
Vol 852 ◽  
pp. 199-204
Author(s):  
Qing Rong Yao ◽  
Yi Hao Shen ◽  
Peng Cheng Yang ◽  
Huai Ying Zhou ◽  
Guang Hui Rao ◽  
...  

The effect of temperature on the structural evolution and physical properties of nanocrystalline BiFeO3 compound has been studied systematically. The results show that the compound crystallizes in the hexagonal LiNbO3 type-structure (space group R3c) and the structural characterization was a=b=5.5979 Å, c=13.9163 Å and V=387.43 Å3. The average crystallite size was about 32.5 nm. The Neel temperature was the same in the vacuum and air conditions, but the decomposition temperature in the air condition was higher 190°C than that of the vacuum condition.


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