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1.
The limits of miscibility within a portion of the system Na2 O-ZnO-B2 O3 -SiO2 were determined at 650°, 800°, and 950°C. The miscibility gap at 800° and 950°C is a low dome, adjoining the zinc borosilicate miscibility gap. Below 755°C the dome intersects the Na2O-B2 O3 -SiO2 face of the phase diagram. The locus of this intersection is in agreement with literature data on the sodium borosilicate system. Estimated tie-line placement in the ZnO-B2 O3 -SiO2 miscibility gap at 1300°C resembles those reported for the corresponding CaO and SrO systems. The microscopic morphology of glasses with the weight composition xNa2 O-18ZnO-18B2 O3 -64SiO2 with 0≤×≤12 is described in detail. 相似文献
2.
Daniele Mazza Mario Vallino Guido Busca 《Journal of the American Ceramic Society》1992,75(7):1929-1934
A morphous solids belonging to the systems Al2 O3 –Me2 O (Me = Na, K) and Al2 O3 –B2 O3 were prepared by nitrate decomposition, introducing boron in the form of boric acid. Crystalline metastable solids with pseudotetragonal symmetry were obtained from thermal treatment at 850° to 900°C for the compositions Al6 Mex O(9+0.5 x ) ( x ≅ 1; Me = Na, K) and Al6- x B x O9 (1 x 3). The resultant solids were stable only within a difinite temperature range and transformed, with further treatment increases, into stable equilibrium phases. The structures of the metastable phases were examined by X-ray diffraction and Fourier transform infrared spectroscopy, and both analyses showed a mullite type of framework, inside of which the atomic coordinates were refined in the Pbam (no. 55) space group. The present results indicate that these silica-free mullite structures are stabilized by two different mechanisms: (1) interstitial occupation of bulky cations (Na+ , K+ ) or (2) substitution of B for Al in some of the tetrahedral positions. 相似文献
3.
The subliquidus miscibility gap in the system K2 O-B2 O3 -SiO2 has been determined for compositions with molar ratios SiO2 /B2 O3 <2 and T≥550°C. The shape of the miscibility gap is an elongated dome similar in form to, but less extensive than those in the lithium and sodium borosilicate systems. The consolute composition (molar) and temperature are estimated to be 4 ± 1 K2 O -30±8 B2 O3 -66±8 SiO2 and 629±5°C, respectively . 相似文献
4.
MASAHIRO TATSUMISAGO AKIRA HAMADA TSUTOMU MINAMI MASAMI TANAKA 《Journal of the American Ceramic Society》1983,66(2):117-119
Twin-roller quenching produced wide ranges of glass formation in the systems Li2 O-RO-Nb2 O5 (R=Ba,Ca,Mg). The glass-forming ability is improved with an increase in the ionic radius of R2+ ions. The crystallization temperature is increased as Li2 O is replaced by RO or the ionic radius of R2+ ions is increased. Infrared spectra revealed that the glass LiNbO3 (=50Li2 O-0Nb2 O5 ) was composed of six-coordinated NbO6 octahedra, which were joined together by corner-sharing only. In the Li2 O-RO-Nb2 O5 glasses there exist edge-shared as well as corner-shared NbO6 octahedra. The edge-shared NbO6 octahedra in the glasses are increased with an increase in the content of RO or Nb2 O5 , and also with an increase in the ionic radius of R2+ ions. 相似文献
5.
S. Y. Limaye ast; D. K. Agrawal ast; H. A. Mckinstry 《Journal of the American Ceramic Society》1987,70(10):232-C
MZr4 P6 O24 (M=Mg, Ca, Sr, Ba), which belongs to a new, low-thermal-expansion family of materials known as [NZP] or [CTP], were synthesized by solid-state reaction (oxide mixing) and sol-gel methods, and their sinterability in two cases was investigated and compared. Thermal-expansion measurements were made on sintered samples by dilatometry, high-temperature X-ray diffractometry, and the laser speckle technique. An anisotropy in axial thermal-expansion coefficients was observed in these materials. CaZr4 P6 O24 and SrZ4 P6 O24 showed reverse anisotropy as well as opposite bulk thermal expansion; i.e., CaZr4 P6 O24 had negative bulk thermal expansion and SrZr4 P6 O24 positive bulk thermal expansion in the temperature range 25° to 500°C. The microstructure of the sintered samples was also examined by scanning electron microscopy. 相似文献
6.
An unambiguous definition is proposed for the thermal efficiency of a fuel-fired, ohmically heated, or combination furnace melting a glass of any com- position. 相似文献
7.
CECIL M. JONES II 《Journal of the American Ceramic Society》1971,54(7):347-349
A technique for growing α-Al2 O3 crystals is described in which Na2 O·11Al2 O3 is dissolved in a liquid of composition Na2 O·4TiO2 ·3Al2 O3 . Alpha Al2 O3 is precipitated as Na2 O evaporates from the system; Na2 O·11Al2 O3 serves as a source of Al2 O3 , and Na2 O in the liquid. The content of solids in the mixture is always such that it does not melt completely. The size of the α-Al2 O3 crystals grown is related to the Na2 O content of the composition. Crystals as large as 4000 by 3000 μm in the α-axis direction and 500 μm in the c -axis direction have been grown. 相似文献
8.
Alumina and gallia were substituted separately for Na2 O in amounts of 0.2, 0.5, 1.0, 1.5, 2.0, and 3.0 wt% in three Na2 O-SiO2 glass compositions (82, 84, and 86 wt% SiO2 ) within the immiscibility region. The immiscibility regions for each system extend to ∼1.5 mol% of the added oxide. In general, the addition reduced the immiscibility temperature ( T m ), but at the edge of the immiscibility region (82% SiO2 ) the Na2 O loss effect initially increased T m . A structural model of the miscibility of Al2 O3 added to silicate glasses is presented. 相似文献
9.
L. M. FOSTER G. V. CHANDRASHEKHAR J. E. SCARDEFIELD R. B. BRADFORD 《Journal of the American Ceramic Society》1980,63(9-10):509-512
A new phase diagram for the system Na2 O-Ga2 O3 (>50 mol% Ga2 O3 ) is presented. It is based on information from differential thermal analysis, X-ray examination of quenched samples, and a radiochemical technique for determining the compositions of a primary phase and a liquid in equilibrium with it. The diagram provides a guide for the growth of primary crystals of the two ionically conducting sodium gallates that are analogs of the technologically important β- and β"-aluminas. 相似文献
10.
E. F. RIEBLING 《Journal of the American Ceramic Society》1974,57(9):373-377
Ternary Na2 O.Sb2 O3 .GeO2 glasses (with various [Na]/[Na + Sb] ratios) that contained ≥65 mol% GeO2 were prepared. Their densities (volumes), refractive indices, and infrared spectra were determined and their colors noted. The ternary glasses with ≥88 mol% GeO2 exhibit nearly additive volumes, refractivities, and frequencies for the main Ge-O vibration. Ternary glasses with lesser amounts of GeO2 exhibit a variety of behaviors, depending on the [Na]/[Na + Sb] ratio. Small amounts of Sb2 O3 cause significant volume and refraction deviations, as well as changes in νGe-O , that can be associated with gradual elimination of GeO6 octahedra. All the information supports a model for the glasses with 65 to 88 mol% GeO2 that involves a degree of depolymerization that is greater when Na2 O and Sb2 O3 are present together than when either is present alone. 相似文献
11.
Phase equilibria data, obtained both by differential thermal analysis and by quenching, are presented for the system Na2 O-Nb2 O5 . Five compounds corresponding to the formulas 3Na2 O.1Nb2 06 , lNa2 O. 1Nb2 O5 , lNa2 O 4Nb2 O6 , lNaz O.7Nb2 O5 , and lNa2 O. 10Nb2 O6 have been found. The compound 3Naz 0.lNb2 O5 melts congruently at 992°C. The compounds 1Na2 O. 4Nb2 O6 , lNa2 O.7Nb2 O, and 1Na2 O. 1Onb2 O5 melt incongruently at 1265°, 1275°, and 1290°C., respectively. The well-known perovskite structure phase NaNbO3 was found to melt congruently at 1412°C. The transition temperatures in NaNbO5 were checked by thermal analysis and only the major structural changes at 368° and 640°C. could be detected. A new disordered form of NaNbO3 could be preserved to room temperature by very rapid quenching. 相似文献
12.
MADELEINE H. WARZEE MARCEL MAURICE FRANZ HALLA WALTER R. RUSTON 《Journal of the American Ceramic Society》1965,48(1):15-17
In the binary system PbO–Laz O3 only one compound, 4PbO.La2 O3 , exists; it is flanked by two eutectics. The structure of the compound, although of lower symmetry, is intimately related to the C modification of the rare earths. Below 800° to 1000°C, metastable solid solutions are formed from oxide mixtures coprecipitated from mixed solutions of the nitrates, the cubic parameter a = 5.66 A, if extrapolated to pure La2 O3 , corresponding to half the a parameter of the C form of La2 O3 . The solid solutions existing between the compositions La2 O3 –2Pb0 and pure La2 O3 have a cubic face–centered lattice and obey Vegard's rule. The systems of PbO with Sm2 O3 and Gd2 O8 are quite similar to that with La2 O3 . The compound Sm2 O3 .4Pb0 decomposes at 1000°C with evaporation of PbO; Sm2 O3 remains in the B modification. 相似文献
13.
Phase relations in the system Na2 O· Al2 O3 -CaO· Al2 O3 -Al2 O3 at 1200°C in air were determined using the quenching method and high-temperature X-ray diffraction. The compound 2Na2 O · 3CaO · 5Al2 O3 , known from the literature, was reformulated as Na2 O · CaO · 2Al2 O3 . A new compound with the probable composition Na2 O · 3CaO · 8Al2 O3 was found. Cell parameters of both compounds were determined. The compound Na2 O · CaO-2Al2 O3 is tetragonal with a = 1.04348(24) and c = 0.72539(31) nm; it forms solid solutions with Na2 O · Al2 O3 up to 38 mol% Na2 O at 1200°C. The compound Na2 O · 3CaO · 8Al2 O3 is hexagonal with) a = 0.98436(4) and c = 0.69415(4) nm. The compound CaO · 6Al2 O3 is not initially formed from oxide components at 1200°C but behaves as an equilibrium phase when it is formed separately at higher temperatures. The very slow transformation kinetics between β and β "-Al2 O3 make it very difficult to determine equilibrium phase relations in the high-Al2 O3 part of the diagram. Conclusions as to lifetime processes in high-pressure sodium discharge lamps can be drawn from the phase diagram. 相似文献
14.
Kentaro Terashima Sae-Hoon Kim Toshinobu Yoko 《Journal of the American Ceramic Society》1995,78(6):1601-1605
The third-order nonlinear optical susceptibilities χ(3) of M2 O-B2 O3 (M = Li, Na, K, Rb, Cs, and Ag) binary borate glasses have been measured by the third harmonic generation (THG) method. It is found that the enhancement of χ(3) by the structural change of BO3 units to BO4 units is small, while the enhancement of χ(3) due to the formation of non- bridging oxygen is rather significant. The effects of alkali cations on the χ(3) of alkali borate glasses are discussed in terms of the M-O bond character, focusing on the covalency of Li2 O-B2 O3 glasses. Comparison of the χ(3) values for Cs2 O-B2 O3 and Ag2 O-B2 O3 glasses which contain cations of comparable polarizability reveals that the χ(3) value is much greater for Ag2 O-B2 O3 glasses than for Cs2 O-B2 O3 glasses, which is possibly due to the great contribution of Ag(4 dz2 + 5 s + 5 pz ) hybrid orbitals to the nonlinear optical response. 相似文献
15.
Phase relationships in the system Li2O, B2O3-B2O3 were studied by the quenching method using twenty compositions. The crystalline phases encountered were (a) Li2O, B2O3, which melts congruently at 849°± 2°C., (b) Li2O.-2B2O3, which melts congruently at 917°± 2°C., (c) a new compound, 2Li2O-5B2O3, which melts incongruently at 856°± 2°C. and dissociates below 696°± 4°C., (d) Li2O.3B2O3, which melts incongruently at 834°± 4°C. and dissociates below 595°± 20°C., and (e) probably Li2O.4B2O3, which melts incongruently at 635°± 10°C. Reactions were sluggish at temperatures near 600°C., resulting in metastable relations. Hence phase equilibrium data relating to the lower stability limit of Li2O.3B2O3 and to the upper stability limit of Li2O.4B2O3 are considered to be tentative. Properties of the glasses and crystalline phases were studied. The refractive index of the glasses increased with the addition of Li2O up to 22%, but further additions up to 40% had no substantial effect. Glasses containing less than 30% Li2O were water soluble. Limited data on the density and thermal expansion of the glasses are presented. Li2OB2O3 was euhedral, lath-shaped, length-fast, biaxial negative (2V = 27°), with nα= 1.540, nβ= 1.612, nγ= 1.616. Li2O.2B2O3 was uniaxial negative, with ne= 1.560, nw= 1.605. Li2O.3B2O3 was biaxial negative (2V = 75° to 80°), with nα= 1.576, nβ= 1.602, nγ= 1.605. X-ray powder diffraction data for the five crystalline compounds are presented. Thermal expansion data for Li2O-B2O3 and Li2O.2B2O3 and limited data on the fluorescent properties of the compounds are given. X-ray diffraction data are also presented for Li2O.B2O3.4H2O and Li2O.-5B2O3. 10H2O. Li2O B2O3 was obtained by heating the first hydrate at 450° to 680° C. X-ray diffraction showed Li2O.4B2O3 and Li2O-3B2O3 to be the crystalline products obtained during heating the decahydrate at 500°C. and 600°C., respectively. 相似文献
16.
MARIA ISABEL NIETO ALICIA DURAN JOSE MARIA FERNANDEZ NAVARRO JOSE LUIS OTEO MAZO 《Journal of the American Ceramic Society》1984,67(4):242-244
Infrared spectra of glasses of the system R2 O-B2 O3 -SiO2 were investigated. The extinction coefficients of the hydroxyl absorption band ("free OH") were calculated by a method proposed for alkali borate glasses. The results confirmed the applicability of this method to homogeneous and phase-separated alkali borosilicate glasses. The variation of the hydroxyl absorption band position was interpreted according to the structural characteristics of the studied glasses. 相似文献
17.
18.
Europium sesquioxide is of interest as a control material for reactors because it has several large-cross-section isotopes which form successively on neutron capture. Pure monoclinic Eu2 O3 tends to grow large grains during sintering, causing microcracks to develop and leading to anomalous mechanical properties. The effect of doping the Eu2 O3 with the grain growth suppressant Ta2 O3 was determined using studies of the elastic properties and internal friction by the sonic resonance technique. Compositions with <3 at.% Ta cation substitution had anomalously low room temperature elastic moduli values and showed a hysteresis on thermal cycling. These specimens also had high internal frictions. The finer-grained specimens which resulted when the dopant level exceeded 3 at.% Ta did not show these anomalous characteristics. 相似文献
19.
In an attempt to understand the liquid–liquid phase separation in the B2 O3 –MgO, B2 O3 –CaO, B2 O3 –SrO, and B2 O3 –BaO systems, the liquid miscibility gaps were calculated using the optimized interaction parameters of liquid phases. The Gibbs energies of liquid phases were derived in the form of a subregular solution from an optimization procedure based on phase diagram data. In addition, metastable liquidus boundaries and spinodal curves were also assessed by using the Gibbs energies of liquid phases. The present results were compared and discussed with other experimental and assessed data available in the literature. 相似文献