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1.
The subsolidus phase relations in the entire system ZrO2 -Y2 O3 were established using DTA, expansion measurements, and room- and high-temperature X-ray diffraction. Three eutectoid reactions were found in the system: ( a ) tetragonal zirconia solid solution→monoclinic zirconia solid solution+cubic zirconia solid solution at 4.5 mol% Y2 O3 and ∼490°C, ( b ) cubic zirconia solid solutiow→δ-phase Y4 Zr3 O12 +hexagonalphase Y6 ZrO11 at 45 mol% Y2 O3 and ∼1325°±25°C, and ( c ) yttria C -type solid solution→wcubic zirconia solid solution+ hexagonal phase Y6 ZrO11 at ∼72 mol% Y2 O3 and 1650°±50°C. Two ordered phases were also found in the system, one at 40 mol% Y2 O3 with ideal formula Y4 Zr3 O12 , and another, a new hexagonal phase, at 75 mol% Y2 O3 with formula Y6 ZrO11 . They decompose at 1375° and >1750°C into cubic zirconia solid solution and yttria C -type solid solution, respectively. The extent of the cubic zirconia and yttria C -type solid solution fields was also redetermined. By incorporating the known tetragonal-cubic zirconia transition temperature and the liquidus temperatures in the system, a new tentative phase diagram is given for the system ZrO2 -Y2 O3 . 相似文献
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MEZAME SHIBATA-YANAGISAWA MASAHARU KATO HIROSHI SETO NOBUO ISHIZAWA NOBUYASU MIZUTANI MASANORI KATO 《Journal of the American Ceramic Society》1987,70(7):503-509
The crystallography of diffusion-induced and diffusionless cubic-to-tetragonal phase transformations in the ZrO2 -Y2 O3 system is examined on the basis of the phenomenological crystallographic theory by adopting the lsqb;011rsqb; (0 1 1) twinning system as the lattice invariant deformation system. Numerical calculation indicates that the principal axes of the cubic phase are not exactly parallel to those of the tetragonal phase and that the habit plane orientation is sensitive to the lattice parameters of the cubic and tetragonal phases. The calculated results are compared with the observed crystallography of the tetragonal precipitates formed by diffusion and of the metastable tetragonal phase formed in a diffusionless manner. In many aspects, the present results were in good agreement with experimental observations. In particular, the crystallography and morphology of the so-called "herringbone" structure are very well explained by the present analysis. 相似文献
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The tetragonal ( t ) and cubic ( c ) ZrO2 solid solutions in two-phase ZrO2 -8 wt% Y2 O3 ceramics have low and high solute content, respectively. Annealing samples sintered at 1600°C between 700° and 1400°C requires a change in the volume fraction of the coexisting phases, as well as their equilibrium Y2 O3 content. The enrichment in Y2 O3 content of the c -ZrO2 grains is accomplished by liquid-film migration involving the ubiquitous silicate grain-boundary phase, while the volume fraction of t -ZrO2 increases by the nucleation and growth of cap-shaped t -ZrO2 lenses. The interfaces between the c -ZrO2 matrix and the growing t -ZrO2 lenses are semicoherent. 相似文献
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F.F. LANGE 《Journal of the American Ceramic Society》1986,69(3):240-242
The average grain size of ZrO2 (+Y, o,) materials sintered at 1400°C was observed to depend significantly on the Y2 O3 content. The average grain size decreased by a factor of 4 to 5 for Y2 O3 contents between 0.8 and 1.4 mol% and increased at Y2 O3 contents of 6.6 mol%. Grain growth control by a second phase is the concept used to interpret these data; compositions with a small grain size lie within the two-phase tetragonal + cubic phase field, and the size of the tetragonal grains is believed to be controlled by the cubic grains. This interpretation suggests that the Y2 O3 -rich boundary of the two-phase field lies between 0.8 and 1.4 mol% Y2 O3 . Transformation toughened materials fabricated in this binary system must have a composition that lies within the two-phase field to obtain the small grain size required, in part, to retain the tetragonal toughening agent. 相似文献
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TAKAKI MASAKI 《Journal of the American Ceramic Society》1986,69(8):638-640
Tetragonal zirconia polycrystals were produced from high-purity powders containing 1.5 to 5.0 mol% Y2 O3 by cold isostatic pressing and sintering, hot-pressing, and hot isostatic pressing. The mechanical properties and microstructures of these resulting materials were examined, with emphasis on the relation between strength and fracture toughness. 相似文献
7.
Phase equilibria in the system MgO-B2 O3 were investigated using DTA and quenching techniques. The system contains 4 invariant points. The compounds MgO·2B2 O3 and 2MgO·B2 O3 melt incongruently at 995° and 1312°C, respectively, whereas 3MgO·B2 O3 melts congruently at 1410°C. A eutectic occurs at 1333°C and 71% MgO. 相似文献
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THOMAS L. BARRY V. S. STUBICAN RUSTUM ROY † 《Journal of the American Ceramic Society》1966,49(12):667-670
Phase equilibrium relations in the system CaO-Yb2 O3 were studied. Results of this work demonstrated the existence of four crystalline phases: Yb2 O3 .3CaO, Yb2 O3 .2CaO, Yb2 O3 °CaO, and 2Yb2 O3 °CaO. The 2Yb2 O3 °CaO phase is metastable at all temperatures and was obtained only by rapid quenching from the melt. The crystalline solubility limit of Yba O3 in CaO at 1850°C is slightly greater than 8 mole %, whereas no solubility of CaO in Yb2 O3 was detected. All four compounds have subsolidus minimums of stability and dissociate into the component oxides below 1800°C. Data are also presented for the systems CaO-Gd2 O3 and CaO-La2 O3 . 相似文献
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The phase equilibria in the zirconia-rich part of the system ZrO2 −Yb2 O3 −Y2 O3 were determined at 1200°, 1400°, and 1650°C. The stabilizing effects of Yb2 O3 and Y2 O3 were found to be quite similar with <10 mol% of either being necessary to fully stabilize the cubic fluorite-structure phase at 1200°C. The two binary ordered phases, Zr3 Yb4 O12 and Zr3 Y4 O12 , are completely miscible at 1200°C. These were the only binary or ternary phases detected. The ionic conductivities of ternary specimens in this system were measured using the complex impedance analysis technique. For a given level of total dopant, the substitution of Yb2 O3 for Y2 O3 gives only minor increases in specimen conductivity. 相似文献
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Doreen D. Edwards Pollyanna E. Folkins Thomas O. Mason 《Journal of the American Ceramic Society》1997,80(1):253-257
Subsolidus phase relationships in the Ga2 O3 –In2 O3 system were studied by X-ray diffraction and electron probe microanalysis (EPMA) for the temperature range of 800°–1400°C. The solubility limit of In2 O3 in the β-gallia structure decreases with increasing temperature from 44.1 ± 0.5 mol% at 1000°C to 41.4 ± 0.5 mol% at 1400°C. The solubility limit of Ga2 O3 in cubic In2 O3 increases with temperature from 4.X ± 0.5 mol% at 1000°C to 10.0 ± 0.5 mol% at 1400°C. The previously reported transparent conducting oxide phase in the Ga-In-O system cannot be GaInO3 , which is not stable, but is likely the In-doped β-Ga2 O3 solid solution. 相似文献
11.
Zirconia-rich subsolidus phase relationships in the ZrO2 –Sc2 O3 and ZrO2 –In2 O3 systems were investigated. Phase inconsistencies in the ZrO2 –Sc2 O3 system resulted from a diffusionless cubic-to-tetragonal ( t' ) phase transformation not being recognized in the past. Through three different measuring techniques, along with microstructural observations, the solubility limits of the tetragonal and cubic phases were determined. 相似文献
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Strength and fracture toughness results are presented for ZrO2 single crystals stabilized with Y2 O3 . The crystals (2 cm in diameter by 5 cm long) were prepared by skull melting. The partially stabilized compositions with 4 to 6 wt% Y2 O3 showed a dramatic improvement in mechanical properties over the fully stabilized samples containing 20 wt% Y2 O3 , i.e. a strength exceeding 1000 MPa and a fracture toughness of 8 Mpa,.m 1/2 were achieved compared to 200 MPa and 2 Mpa.m1/2 , respectively, for fully stabilized ZrO2 single crystals. 相似文献
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The phase diagram for the system NdI2 O3 -P2 O5 was constructed. Six intermediate compounds, having molar Nd2 O3 : P2 O5 ratios of 3:1, 7:3, 1:1, 1:2, 1:3, and 1:5, were identified. The 3:1, 7:3, and 1:1 compounds are stable to at least 1500°C. The 1:2 compound decomposes to 1:1 and 1:3 at 730 ± 5°C. The 1:3 and 1:5 compounds melt congruently at 1280 ± 5° and 1055 ± 5°C, respectively. None of the neodymium phosphates show lower temperature limits of stability. 相似文献
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Subsolidus phase equilibria in the system La2 O3 -P2 O5 were established. The system contains six intermediate compounds having molar La2 O3 :P2 O5 ratios of 3:1,7:3,1:1,1:2,1:3, and 1:5. It was found that the 3:1 compound has a phase transformation at 935°C. The 1:2 compound decomposes to a mixture of 1:1 and 1:3 at 755°C. The 1:3 compound melts incongruently to 1:1 and liquid at 1235°C and the 1:5 compound melts congruently at 1095°C. None of the lanthanum phosphates have lower temperature limits of stability. 相似文献
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The existence of stable and metastable forms of 2ZrO2 ·P2 O5 and the subsolidus phase relations in the system ZrO2 -ZrP2 O7 were confirmed before investigation of the ternary system. The synthesis and thermal behavior of ZrW2 O8 were reinvestigated, and the system WO3 -P2 O5 was examined cursorily. A ternary compound, 2ZrO2 ·WO3 ·P2 O5 , was found, and compatibility triangles for the system between 1105° and 1150°C were established. The ternary compound is compatible with ZrO2 , WO3 , and three binary compounds, giving rise to five composition triangles. In addition, ZrP2 O7 , WO3 , and "W2 O3 (PO4 )2 " were compatible. 相似文献
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《Journal of the American Ceramic Society》1979,62(3-4):212-214
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Phase equilibria in the system SrO-CdO-V2 O5 in air were established from data obtained by DTA, quenching, and high-temperature solid-state reaction experiments. The SrO-V2 O5 boundary system contains 4 compounds at SrO to V2 O5 molar ratios of 4:1, 3:1, 2:1, and 1:1. A fifth compound with a molar composition of ∼10:3 with the apatite crystal structure was also found; it may, however, be a hydroxyapatite phase. The CdO-V2 O5 system contains the compounds 3CdO·V2 O5 , 2CdO·V2 O5 , and CdO·V2 O5 . The latter compound exhibits a rapid reversible polymorphic transition at 180°C. Complete solid solubility exists in the SrO-CdO system. The most probable compatibility relations were determined from the data available for the SrO-CdO-V2 O5 ternary system. Limited solid solubility exists between SrO·V2 O5 and CdO·V2 O5 , and the high-temperature CdO·V2 O5 polymorph is stabilized to room temperature by solid solution of SrO·V2 O5 . Evidence for the existence of 2 ternary compounds with limited local solid solubility is also presented. 相似文献
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The subsolidus compatibility relations in the system SrO-B2 O3 - SiO2 were determined by solid-state reaction techniques and X-ray powder diffraction methods. The system was found to contain 11 subsolidus compatibility relations, one stable ternary compound (Sr3 B2 SiO8 ), and one metastable ternary compound with a probable composition SrB2 Si2 O8 . 相似文献
20.
Elena R. Andrievskaya Lidia M. Lopato Vasily P. Smirnov 《Journal of the American Ceramic Society》1996,79(3):714-720
A mathematical model of the liquidus surface based on a reduced polynomial method was proposed for the system HfO2 -Y2 O3 -Er2 O3 . The results of calculations according to this model agree fairly well with the experimental data. Phase equilibria in the system HfO2 -Y2 O3 -Er2 O3 were studied on melted (as-cast) and annealed samples using X-ray diffraction (at room and high temperatures) and micro-structural and petrographic analyses. The crystallization paths in the system HfO2 -Y2 O3 -Er2 O3 were established. The system HfO2 -Y2 O3 -Er2 O3 is characterized by the formation of extended solid solutions based on the fluorite-type (F) form of HfO2 and cubic (C) and hexagonal (H) forms of Y2 O3 and Er2 O3 . The boundary curves of these solid solutions have the minima at 2370°C (15. 5 mol% HfO2 , 49. 5 mol% Y2 O3 ) and 2360°C (10. 5 mol% HfO2 , 45. 5 mol% Y2 O3 ). No compounds were found to exist in the system investigated. 相似文献