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1.
Phase relations within the "V2 O3 –FeO" and V2 O3 –TiO2 oxide systems were determined using the quench technique. Experimental conditions were as follows: partial oxygen pressures of 3.02 × 10−10 , 2.99 × 10−9 , and 2.31 × 10−8 atm at 1400°, 1500°, and 1600°C, respectively. Analysis techniques that were used to determine the phase relations within the reacted samples included X-ray diffractometry, electron probe microanalysis (energy-dispersive spectroscopy and wavelength-dispersive spectroscopy), and optical microscopy. The solid-solution phases M2 O3 , M3 O5 , and higher Magneli phases (M n O2 n −1 , where M = V, Ti) were identified in the V2 O3 –TiO2 system. In the "V2 O3 –FeO" system, the solid-solution phases M2 O3 and M3 O4 (where M = V, Ti), as well as liquid, were identified. 相似文献
2.
The rate of formation of NiAl2 O4 by reaction between single crystals of NiO and Al2 O3 can be described by k = 1.1 × 104 exp (−108,000 ± 5,000/ RT ) cm2 /s. In NiO the behavior of D as a function of concentration supports the Lidiard theory of diffusion by impurity-vacancy pairs. A good fit of the theory to the experimental results was obtained by assuming that Al3+ ions diffuse as [AlNi · VNi ]'pairs. The diffusion coefficient of pairs, Dp , obeys the equation 6.6 × 10−2 exp (−54,000 ± 3,000/ RT ) cm2 /s. The free energy of association for pairs was calculated to range from 6.5 kcal/mol at 1789°C to 9.0 kcal/mol at 1540°C. The interdiffusion coefficients in the spinel showed a constant small increase with increasing concentration of Al3+ dissolved in the spinel. 相似文献
3.
C. Greskovich 《Journal of the American Ceramic Society》1984,67(6):111-C
The deviation from stoichiometry, δ, in Cr2 −δO3 was measured by a tensivolumetric method in the high pO2 range of ≊104 to 104 Pa at 1100°C. The value of δ, or chromium vacancy concentration, was≊9×10−5 mol/mol Cr2 O3 in air for Cr2 O3 with 99.999% purity. The chemical diffusion coefficient, DT, determined from equilibration data was ≊4.6× cm2 ·s−1 at 1100°C for pO2 = 2.2 ×101 Pa. The self-diffusion coefficient of Cr ions was calculated from and δ and found to be≊1.6×10-17 cm2 -s−1 , in good agreement with recently measured values. 相似文献
4.
The formation of ZnAl2 O4 spinel in diffusion couples of Al2 O3 and ZnO was investigated between 1000° and 1390°C in air and in air containing 4.8 vol% Cl2 by X-ray diffraction, electron probe microanalysis, and scanning electron microscopy. The rate of formation of a spinel layer obeyed a parabolic rate law and was accelerated remarkably by the presence of Cl2 . The interdiffusion coefficient, , and the activation energy, E, were calculated to be 10−8 to 10−9 cm2 /s and 123 kcal/mol (514 kJ/mol) in air and 10−7 cm2 /s and 31 kcal/mol (130 kJ/mol) in air containing 4.8 vol% Cl2 , respectively. 相似文献
5.
Dai Guiqin Lin Wei Zheng An Huang Qingzhen Liang Jingkui 《Journal of the American Ceramic Society》1990,73(8):2526-2527
Thermal expansion of the low-temperature form of BaB2 O4 (β-BaB2 O4 ) crystal has been measured along the principal crystallographic directions over a temperature range of 9° to 874°C by means of high-temperature X-ray powder diffraction. This crystal belongs to the trigonal system and exhibits strongly anisotropic thermal expansions. The expansion along the c axis is from 12.720 to 13.214 Å (1.2720 to 1.3214 nm), whereas it is from 12.531 to 12.578 Å (1.2531 to 1.2578 nm) along the a axis. The expansions are nonlinear. The coefficients A, B , and C in the expansion formula L t = L 0 (1 + At + Bt 2 + Ct 3 ) are given as follows: a axis, A = 1.535 × 10−7 , B = 6.047 × 10−9 , C = -1.261 × 10−12 ; c axis, A = 3.256 × 10−5 , B = 1.341 × 10−8 , C = -1.954 × 10−12 ; and cell volume V, A = 3.107 × 10−5 , B = 3.406 × 10−8 , C = -1.197 × 10−11 . Based on α t = (d L t /d t )/ L 0 , the thermal expansion coefficients are also given as a function of temperature for the crystallographic axes a , c , and cell volume V. 相似文献
6.
CHARLES A. SORRELL 《Journal of the American Ceramic Society》1971,54(10):501-503
Thermal expansion of Pb3 O4 was investigated by high-temperature X-ray diffraction. The coefficient in the a 0 direction is 14.6×10−6 /°C. Expansion in the c0 direction is 32% greater, with a coefficient of 19.3×10−6 /°C. Coefficients of expansion are linear from 25° to 490°C and are comparable with those of tetragonal and orthorhombic PbO. 相似文献
7.
Koji Morita Keijiro Hiraga Yoshio Sakka 《Journal of the American Ceramic Society》2002,85(7):1900-1902
High-strain-rate superplasticity is attained in a 3-mol%-Y2 O3 -stabilized tetragonal ZrO2 polycrystal (3Y-TZP) dispersed with 30 vol% MgAl2 O4 spinel: tensile elongation at 1823 K reached >300% at strain rates of 1.7 × 10−2 – 3.3 × 10−1 s−1 . The flow behavior and the microstructure of this material indicate that the MgAl2 O4 dispersion should enhance accommodation processes necessary for grain boundary sliding. Such an effect is assumed to arise from an enhancement of the cation diffusion by the dissolution of Al and Mg ions into the ZrO2 matrix and from stress relaxation due to the dispersed MgAl2 O4 grains. 相似文献
8.
The compressive creep behavior and oxidation resistance of an Si3 N4 /Y2 Si2 O7 material (0.85Si3 N4 +0.10SiO2 +0.05Y2 O3 ) were determined at 1400°C. Creep re sistance was superior to that of other Si3 N4 materials and was significantly in creased by a preoxidation treatment (1600°C /120 h). An apparent parabolic rate constant of 4.2 × 10−11 kg2 ·m-4 ·s−1 indicates excellent oxidation resistance. 相似文献
9.
Toshiyuki Sata Kazuo Sakai Suguru Tashiro 《Journal of the American Ceramic Society》1991,74(6):1445-1448
Purified air is passed over a specimen of YBa2 Cu3 O7– x at 890°C; the vaporized substances are condensed in a pure alumina tube, then subjected to inductively controlled plasma analysis. Vapor pressure values of 2.5 × 10−5 Pa for BaO( g ), 1.2 × 10−4 Pa for Cu( g ), and 2.2 × 10−5 Pa for CuO( g ) are obtained under 2.1 × 104 Pa (0.21 bar) of oxygen pressure. No Y vapor is detected at this temperature. 相似文献
10.
The electrical conductivity and ion/electron transference numbers in Al3 O3 were determined in a sample configuration designed to eliminate influences of surface and gas-phase conduction on the bulk behavior. With decreasing O2 partial pressure over single-crystal Al2 O3 at 1000° to 1650°C, the conductivity decreased, then remained constant, and finally increased when strongly reducing atmospheres were attained. The intermediate flat region became dominant at the lower temperatures. The emf measurements showed predominantly ionic conduction in the flat region; the electronic conduction state is exhibited in the branches of both ends. In pure O2 (1 atm) the conductivity above 1400°C was σ≃3×103 exp (–80 kcal/ RT ) Ω−1 cm−1 , which corresponds to electronic conductivity. Below 1400°C, the activation energy was <57 kcal, corresponding to an extrinsic ionic condition. Polycrystalline samples of both undoped hot-pressed Al2 O3 and MgO-doped Al2 O3 showed significantly higher conductivity because of additional electronic conduction in the grain boundaries. The gas-phase conduction above 1200°C increased drastically with decreasing O2 partial pressure (below 10−10 atm). 相似文献
11.
The vaporization of the system MgO-Cr2 O3 was studied in a vacuum of 10−5 torr (10−3 N/m2 ) at 1500° to 1700°C using the Langmuir and Knudsen methods. It was found that the phases in the system vaporize nearly congruently and the logarithm of the vaporization coefficient, α, of MgCr2 O4 increases linearly with increasing reciprocal temperature. Alpha tends to unity at a temperature near the melting point (2525±23°C). The additivity rule can be applied to the Langmuir vaporization rates on the basis of the surface area ratios of the phases in the 2-phase system MgO-Cr2 O3 . The enthalpies of vaporization of MgCr2 O4 were 695.0 and 549.2 kcaVmol for activated and equilibrium processes, respectively. 相似文献
12.
The crystal-growth process and growth conditions of β-alumina (Na2 O · Al2 O3 ) were investigated using the Na2 B4 O7 -Na3 AlF6 flux method. β-Alumina (electric fusion brick) was used as both nutrient and seed. Weight loss of the flux varied widely for various runs: ≅ 10 wt% of flux evaporated at 100 h, ≅ 17 wt% at 150 h, and 43 wt% at 600 h. When β-alumina crystal was grown, only 20 wt% Na2 B4 O7 was added to the Na3 AlF6 flux. The linear growth rates of the β-alumina single crystal grown by an Na3 AlF6 -20 wt% Na2 B4 O7 flux method at 1040°C and Δ t = 18°C were ≅ 1.0 × 10−3 mm/h ( a face) and ≅0.3 × 10−3 mm/h ( c face). The β-alumina single crystals grown were bounded by only c [001] and a [100] and were colorless and transparent. 相似文献
13.
The effects of heat treatment in Ar-O2 and H2 -H2 O atmospheres on the flexural strength of hot isostatically pressed Si3 N4 were investigated. Increases in room-temperature strength, to values significantly above that of the aspolished material, were observed when the Si3 N4 was exposed at 1400°C to (1) H2 with water vapor pressure ( P H2O ) greater than 1 × 10−4 MPa or (2) Ar with oxygen partial pressure ( P O2 ) of between 7 × 10−6 and 1.5 × 10−5 MPa. However, the strength of the material was degraded when the P H2O in H2 was lower than 1 × 10−4 MPa, and essentially unaffected when the P O2 in Ar was higher than 1.5 × 10−5 MPa. We suggest that the observed strength increases are the result of strength-limiting surface flaws being healed by a Y2 Si2 O7 layer formed during exposure. 相似文献
14.
C. GRESKOVICH 《Journal of the American Ceramic Society》1970,53(9):498-502
The reaction kinetics for NiCr2 O4 formation and the diffusion of Cr3+ ions into single-crystal NiO were studied between 1300° and 1600°C in air. The experimental activation energy for NiCr2 O4 formation was about 83 kcal/mol. After incubation, NiCr2 O4 formed by a diffusion-controlled process. The origin of pores at the NiO/NiCr2 O4 interface is discussed. The concentration profiles of Cr3+ in NiO were linear because the interdiffusion coefficient was directly proportional to the mol fraction Cr3+ . Theoretical considerations indicate that the interdiffusion coefficient equals 3/2 the self-diffusion coefficient of Cr3+ , which is rate-determining. The interdiffusion coefficient at 1 mol% Cr2 O3 can be expressed as =4×10−3 exp (−55,000/RT) cm2 s−1 . 相似文献
15.
Studies of the oxidation of Gd and Dy at P O2 's from 10−0.3 to 10−14.5 atm and temperatures from 727° to 1327°C indicate both semiconducting and ionic-conducting domains in the sesquioxides formed. At higher temperatures, where dense coarsegrained oxide layers developed, the rate of oxidation in the high- P 02 semiconducting domain yielded oxygen diffusion coefficients in Dy2 O3 in excellent agreement with literature values derived from oxidation of partially reduced oxide single crystals. Under the same conditions, the oxidation of Gd yielded oxygen diffusion coefficients in cubic Gd2 O3 which are considerably below literature values for monoclinic single-crystal Gd2 O3 . At lower temperatures, porous scales were formed, and apparent diffusion coefficients derived from oxidation rates show a smaller temperature dependence than the high-temperature data. At low P O2 , the oxides behave as ionic conductors, and metal oxidation rates result in estimates of the electronic contribution to the electrical conductivity of the order of 10−6 to 10−7 Ω−1 cm−1 . 相似文献
16.
Masahide Okamoto Hironori Kodama Kazuo Shinozaki 《Journal of the American Ceramic Society》2008,91(4):1110-1114
The sintering of a composite of MgO–B2 O3 –Al2 O3 glass and Al2 O3 filler is terminated due to the crystallization of Al4 B2 O9 in the glass. The densification of a composite of MgO–B2 O3 –Al2 O3 glass and Al2 O3 filler using pressureless sintering was accomplished by lowering the sintering temperature of the composite. The sintering temperature was lowered by the addition of small amounts of alkali metal oxides to the MgO–B2 O3 –Al2 O3 glass system. The resultant composite has a four-point bending strength of 280 MPa, a coefficient of thermal expansion (RT—200°C) of 4.4 × 10−6 K−1 , a dielectric constant of 6.0 at 1 MHz, porosity of approximately 1%, and moisture resistance. 相似文献
17.
Kirk A. Rogers Kevin P. Trumble Brian J. Dalgleish Ivar E. Reimanis 《Journal of the American Ceramic Society》1994,77(8):2036-2042
Microstructure development at solid-state diffusion-bonded Cu/α-Al2 O3 interfaces has been studied using optical and electron microscopy. High-purity Cu foil was bonded between basal-oriented α-Al2 O3 single-crystal plates at 1040°C for 24 h in a vacuum of ∼1.3 × 10−4 Pa (1 × 10−6 torr). Optical microscopy of as-bonded specimens revealed a large Cu grain size, fine pores, and long needles of Cu2 O at the interface. Bulk specimens were annealed at 1000°C for various times under controlled oxygen partial pressures in CO/CO2 mixtures. Consistent with a thermochemical analysis, CuAlO2 could be formed at the interfaces. The CuAlO2 was acicular and discontinuous, but occurred in a uniform distribution over the bulk specimen interfaces. 相似文献
18.
Gilles Bussod Alexander Pechenik Chung-tse Chu Bruce Dunn 《Journal of the American Ceramic Society》1989,72(1):137-139
The knowledge of the steady-state stress for plastic deformation as a function of temperature and strain rate is essential for hot-forming superconducting material into commercially useful shapes. In this paper, results are presented on the experimental determination of the rheology of fully dense polycrystalline Y1 Ba2 Cu3 O7−x superconducting material at temperatures ranging from 750° to 950°C and strain rates of 10−4 , 10−5 , and 10−6 s−1 . The data are best fitted by a power law: ε(s−1 )=8.9 × 10−17 . (s−1 ) σ2.5 (Pa) exp [−2.01 × 105 (J·mol−1 )|RT]. X-ray analysis shows that the superconducting material retains its phase composition after nearly 70% total strain of the sample. A strong anisotropy in the resistivity of the deformed samples is observed because of the development of a preferred orientation of the a or b axis of Y1 Ba2 Cu3 O7−x orthorhombic perovskite single crystals perpendicular to the principal maximum compressive stress. 相似文献
19.
Santanu Basu Amitava Chakraborty Parukuttyamma Sujatha Devi Himadri Sekhar Maiti 《Journal of the American Ceramic Society》2005,88(8):2110-2113
Nanocrystalline La0.9 Sr0.1 Al0.85 Co0.05 Mg0.1 O3 oxide powder was synthesized by a citrate–nitrate auto-ignition process and characterized by thermal analysis, X-ray diffraction, and impedance spectroscopy measurements. Nanocrystalline (50–100 nm) powder with perovskite structure could be produced at 900°C by this process. The powder could be sintered to a density more than 96% of the theoretical density at 1550°C. Impedance measurements on the sintered samples unequivocally established the potential of this process in developing nanostructured lanthanum aluminate-based oxides. The sintered La0.9 Sr0.1 Al0.85 Co0.05 Mg0.1 O3 sample exhibited a conductivity of 2.40 × 10−2 S/cm in air at 1000°C compared with 4.9 × 10−3 S/cm exhibited by La0.9 Sr0.1 Al0.85 Mg0.15 O3 . 相似文献
20.
La0.8 Sr0.2 Cr0.9 Ti0.1 O3 perovskite has been designed as an interconnect material in high-temperature solid oxide fuel cells (SOFCs) because of its thermal expansion compatibility in both oxidizing and reducing atmospheres. La0.8 Sr0.2 Cr0.9 Ti0.1 O3 shows a single phase with a hexagonal unit cell of a = 5.459(1) Å, c = 13.507(2) Å, Z = 6 and a space group of R -3 C . Average linear thermal expansion coefficients of this material in the temperature range from 50° to 1000°C were 10.4 × 10−6 /°C in air, 10.5 × 10−6 /°C under a He–H2 atmosphere (oxygen partial pressure of 4 × 10−15 atm at 1000°C), and 10.9 × 10−6 /°C in a H2 atmosphere (oxygen partial pressure of 4 × 10−19 atm at 1000°C). La0.8 Sr0.2 Cr0.9 Ti0.1 O3 perovskite with a linear thermal expansion in both oxidizing and reducing environments is a promising candidate material for an SOFC interconnect. However, there still remains an air-sintering problem to be solved in using this material as an SOFC interconnect. 相似文献