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1.
Advanced sintering techniques for consolidation of Si3N4 powders in the presence of an oxygen-rich liquid phase(s) require high temperatures and usually high nitrogen pressures. A stability diagram is constructed for Si3N4 as a function of the partial pressures of nitrogen (PN2) and silicon (PSi). High PN2 (20 to 100 atm) increases the stability of Si3N4 and the oxygen-rich liquid phase by reducing the PSi and PSi0, respectively. The region of high sinterability is outlined for submicrometer Si3N4 powders containing 7 wt% BeSiN2 and 7 wt% SiO2 as densification aids .  相似文献   

2.
Recent reports in the literature have suggested that Si2N2O forms in the oxidation of Si3N4 as a buffer suboxide below the silica crust, and that equilibrium between SiO2 and Si3N4 requires the presence of this buffer. Here we report the examination of SiO2/Si3N4 boundaries of different genesis, by a variety of techniques, all of which failed to detect Si2N2O. What was found in each case is a graded suboxide whose composition merges seamlessly with the higher oxide above and the Si3N4 below. Part I presents the results of compositional depth profiling across the suboxide. In Part II a model is proposed to explain how O2 diffusion in the graded suboxide limits Si3N4 oxidation kinetics.  相似文献   

3.
Subsolidus phase relations were established in the system Si3N4-SiO2-Y2O3. Four ternary compounds were confirmed, with compositions of Y4Si2O7N2, Y2Si3O3N4, YSiO2N, and Y10(SiO4)6N2. The eutectic in the triangle Si3N4-Y2Si2O7-Y10(SiO4)6N2 melts at 1500°C and that in the triangle Si2N2O-SiO2-Y2Si2O7 at 1550°C. The eutectic temperature of the Si3N4-Y2Si2O7 join was ∼ 1520°C.  相似文献   

4.
The densification behavior of Si3N4 containing MgO was studied in detail. It was concluded that MgO forms a liquid phase (most likely a magnesium silicate). This liquid wets and allows atomic transfer of Si3N4. Evidence of a second-phase material between the Si3N4 grains was obtained through etching studies. Transformation of α- to β-Si3N4 during hot-pressing is not necessary for densification.  相似文献   

5.
The crystal structure of a lutetium silicon oxynitride (Lu4Si2O7N2) was analyzed by the Rietveld method using time-of-flight (TOF) neutron powder diffraction data. The compound crystallizes in a monoclinic cell, space group P 21/ c (No. 14-1) with a = 7.4243(1), b = 10.2728(1), c = 10.6628(1) Å, and β= 109.773(1)° at 297 K. One nitrogen atom in Lu4Si2O7N2 occupies the bridging site between the two Si atoms, and the other one is statistically situated at the terminal sites of Si2O5N2 ditetrahedra. In the local structure, Si2O5N2 ditetrahedra consist of SiO3N and SiO2N2 tetrahedral units sharing the N atom. Lu atoms are in sixfold, sevenfold (×2) and eightfold coordinations of O/N atoms. X-ray powder diffraction data were also analyzed with the model obtained by the neutron diffraction.  相似文献   

6.
The compressive creep behavior and oxidation resistance of an Si3N4/Y2Si2O7 material (0.85Si3N4+0.10SiO2+0.05Y2O3) were determined at 1400°C. Creep re sistance was superior to that of other Si3N4 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   

7.
The dissolution rates of silicon nitride (Si3N4) ceramics into CaOAl2O3SiO2 slags were investigated by using a rotating specimen method in the temperature range of 1773–1873 K. Dissolution rates in the present study increased as the revolution speed and temperature increased and decreased as the SiO2 content of the slags increased. The nitrogen content of the slags increased after the Si3N4 ceramics had been immersed into them. The slags contained two types of nitrogen ions—N3− and CN-—because a graphite crucible was used for the experiment. N3− ions were confirmed in all the slags that were used in the present work; the CN- content was much lower than that of the N3− ions, except in the slag without SiO2. Based on those results, Ficks law of diffusion was used to analyze the dissolution rates. The dissolution mechanism of the Si3N4 ceramics into CaO–Al2O3SiO2 slags has been discussed in this paper.  相似文献   

8.
The rate of dissolution of β-Si3N4 into an Mg-Si-O-N glass was measured by working with a composition in the ternary system Si3N4-SiO2-MgO such that Si2N2O rather than β-Si3N4 was the equilibrium phase. Dissolution was driven by the chemical reaction Si3N4(c)+SiO2( l )→Si2N2O(c). Analysis of the kinetic data, in view of the morphology of the dissolving phase (Si3N4) and the precipitating phase (Si2N2O), led to the conclusion that the dissolution rate was controlled by reaction at the crystal/glass interface of the Si3N4, crystals. The process appears to have a fairly constant activation energy, equal to 621 ±40 kJ-mol−1, at T=1573 to 1723 K. This large activation energy is believed to reflect the sum of two quantities: the heat of solution of β-Si3N4 hi the glass and the activation enthalpy for jumps of the slower-moving species across the crystal/glass interface. The data reported should be useful for interpreting creep and densification experiments with MgO-fluxed Si3N4.  相似文献   

9.
Phase relationships in the Si3N4–SiO2–Lu2O3 system were investigated at 1850°C in 1 MPa N2. Only J-phase, Lu4Si2O7N2 (monoclinic, space group P 21/ c , a = 0.74235(8) nm, b = 1.02649(10) nm, c = 1.06595(12) nm, and β= 109.793(6)°) exists as a lutetium silicon oxynitride phase in the Si3N4–SiO2–Lu2O3 system. The Si3N4/Lu2O3 ratio is 1, corresponding to the M-phase composition, resulted in a mixture of Lu–J-phase, β-Si3N4, and a new phase of Lu3Si5ON9, having orthorhombic symmetry, space group Pbcm (No. 57), with a = 0.49361(5) nm, b = 1.60622(16) nm, and c = 1.05143(11) nm. The new phase is best represented in the new Si3N4–LuN–Lu2O3 system. The phase diagram suggests that Lu4Si2O7N2 is an excellent grain-boundary phase of silicon nitride ceramics for high-temperature applications.  相似文献   

10.
The influence of phase formation on the dielectric properties of silicon nitride (Si3N4) ceramics, which were produced by pressureless sintering with additives in MgO–Al2O3–SiO2 system, was investigated. It seems that the difference in the dielectric properties of Si3N4 ceramics sintered at different temperatures was mainly due to the difference of the relative content of α-Si3N4, β-Si3N4, and the intermediate product (Si2N2O) in the samples. Compared with α-Si3N4 and Si2N2O, β-Si3N4 is believed to be a major factor influencing the dielectric constant. The high-dielectric constant of β-Si3N4 could be attributed to the ionic relaxation polarization.  相似文献   

11.
The rates of densification and phase transformation undergone by α-Si3N4 during hot-pressing in the presence of Y2O3, Y2O3−2SiO2, and Li20−2Si02 as additives were studied. Although these systems behave less simply than MgO-doped Si3N4, the data can be interpreted during the early stages of hot-pressing as resulting from a solution-diffusion-reprecipitation mechanism, where the diffusion step is rate controlling and where the reprecipitation step invariably results in the formation of the β-Si3N4 phase.  相似文献   

12.
The results of two-step oxidation experiments on chemically-vapor-deposited Si3N4 and SiC at 1350°C show that a correlation exists between the presence of a Si2N2O interphase and the strong oxidation resistance of Si3N4. During normal oxidation, k p for SiC was 15 times higher than that for Si3N4, and the oxide scale on Si3N4 was found by SEM and TEM to contain a prominent Si2N2O inner layer. However, when oxidized samples are annealed in Ar for 1.5 h at 1500°C and reoxidized at 1350°C as before, three things happen: the oxidation k p increases over 55-fold for Si3N4, and 3.5-fold for SiC; the Si3N4 and SiC oxidize with nearly equal k p's; and, most significant, the oxide scale on Si3N4 is found to be lacking an inner Si2N2O layer. The implications of this correlation for the competing models of Si3N4 oxidation are discussed.  相似文献   

13.
Phase relation studies of Si3N1, SiO2, and MgO have established three important subsolidus tie lines, viz. Si3N4-MgO, Si3N4-Mg2SiO4, and Si2N2O-Mg2SiO4 for nonoxidizing fabrication conditions. Strength measurements at 1400°C show that optimum strengths are obtained for compositions approaching the Si3N4-MgO and Si3N4-Si2N2O tie lines and that inferior strengths are obtained for compositions approaching the Si3N4-Mg2SiO4 tie line. Oxidation measurements at 1375°C show that the oxidation kinetics depend on the content of MgO and Mg2SiO4 phases. Optimum oxidation resistance is observed for compositions approaching the Si3N4-Si2N2O tie line. Strength and oxidation results are discussed with regard to phase equilibrium considerations.  相似文献   

14.
The 1780°C isothermal section of the reciprocal quasiternary system Si3N4-SiO2-BeO-Be3N2 was investigated by the X-ray analysis of hot-pressed samples. The equilibrium relations shown involve previously known compounds and 8 newly found compounds: Be6Si3N8, Be11Si5N14, Be5Si2N6, Be9Si3N10, Be8SiO4N4, Be6O3N2, Be8O5N2, and Be9O6N2. Large solid solubility occurs in β-Si3N4, BeSiN2, Be9Si3N10, Be4SiN4, and β-Be3N2. Solid solubility in β-Si3N4 extends toward Be2SiO4 and decreases with increasing temperature from 19 mol% at 1770°C to 11.5 mol% Be2SiO4 at 1880°C. A 4-phase isotherm, liquid +β-Si3N4 ( ss )Si2ON2+ BeO, exists at 1770°C.  相似文献   

15.
The oxidation behaviors of monolithic Si3N4 and nanocomposite Si3N4-SiC with Yb2O3 as a sintering aid were investigated. The specimens were exposed to air at temperatures between 1200° and 1500°C for up to 200 h. Parabolic weight gains with respect to exposure time were observed for both specimens. The oxidation products formed on the surface also were similar, i.e., a mixture of crystalline Yb2Si2O7 and SiO2 (cristobalite). However, strength retention after oxidation was much higher for the nanocomposite Si3N4-SiC compared to the monolithic Si3N4. The SiC particles of the nanocomposite at the grain boundary were effective in suppressing the migration of Yb3+ ions from the bulk grain-boundary region to the surface during the oxidation process. As a result, depletion of yttribium ions, which led to the formation of a damaged zone beneath the oxide layer, was prevented.  相似文献   

16.
The oxidation behavior and its effect on the mechanical properties of fibrous monolith Si3N4/BN after exposure to air at temperatures ranging from 1000° to 1400°C for up to 20 h were investigated. After exposure at 1000°C, only the BN cell boundary was oxidized, forming a B2O3 liquid phase. With increasing exposure temperature, the Si3N4 cells began to oxidize, forming crystalline Y2Si2O7, SiO2, and silicate glass. However, in this case, a weight loss was observed due to extensive vaporization of the B2O3 liquid. After exposure at 1400°C, large Y2Si2O7 crystals with a glassy phase formed near the BN cell boundaries. The oxidation behavior significantly affected the mechanical properties of the fibrous monolith. The flexural strength and work-of-fracture decreased with increasing exposure temperature, while the noncatastrophic failure was maintained.  相似文献   

17.
The subsolidus phase relationships in the system Si,Al,Y/N,O were determined. Thirty-nine compatibility tetrahedra were established in the region Si3N4─AIN─Al2O3─Y2O3. The subsolidus phase relationships in the region Si3N4─AIN─YN─Y2O3 have also been studied. Only one compound, 2YN:Si3N4, was confirmed in the binary system Si3N4─YN. The solubility limits of the α'─SiAION on the Si3N4─YN:3AIN join were determined to range from m = 1.3 to m = 2.4 in the formula Y m /3Si12- m Al m N16. No quinary compound was found. Seven compatibility tetrahedra were established in the region Si3N4─AIN─YN─Y2O3.  相似文献   

18.
Full-density Si3N4-SiO2-Ce2O3 compositions were prepared by sintering with 2.5 MPa nitrogen pressure at temperatures of 1900° and 2090°C. Room-temperature flexural strengths near 700 MPa for sintered material compared favorably with the strength of hot-pressed material. At 1370°C, where flexural strengths as high as 363 MPa were obtained, it was observed that the coarsest structure was the strongest and the finest structure was the weakest. One of the compositions tested, Si3N4-8.7 wt% SiO2-8.3 wt%-Ce2O3, was found to have excellent 200-h oxidation resistance at 700°, 1000°, and 1370°C, without incidence of 700° to 1000°C phase instability and cracking.  相似文献   

19.
Si3N4 substrates coated with chemically-vapor-deposited, crystalline mullite (3Al2O3.2SiO2) were subjected to a corrosive environment containing Na2SO4 and O2 at 1000°C for 100 h. The composition and microstructure of the as-deposited and corroded specimens were examined and compared. The coating appeared to be effective in preserving and therefore protecting the surface microstructure of the underlying Si3N3 substrates. However, a small degree of Na penetration through mullite grain boundaries was observed to a coating depth of ∼1 μm.  相似文献   

20.
The synthesis and structure of a monodispersed spherical Si3N4/SiC nanocomposite powder have been studied. The Si3N4/SiC nanocomposite powder was synthesized by heating under argon a spherical Si3N4/C powder. The spherical Si3N4/C powder was prepared by heating a spherical organosilica powder in a nitrogen atmosphere and was composed of a mixture of nanosized Si3N4 and free carbon particles. During the heat treatment at 1450°C, the Si3N4/C powder became a Si3N4/SiC composite powder and finally a SiC powder after 8 h, while retaining its spherical shape. The composition of the Si3N4/SiC composite powder changed with the duration of the heat treatment. The results of TEM, SEM, and selected area electron diffraction showed that the Si3N4/SiC composite powder was composed of homogeneously distributed nanosized Si3N4 and SiC particles.  相似文献   

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