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1.
Extended x-ray-absorption fine structure and scanning electron microscopy have been applied to the structure of the vanadium oxide layers on impregnated and grafted vanadium aerosils. When aerosil is impregnated with NH4VO3 solution, V2O5 crystals are formed; when vanadium is grafted by reacting the oxychloride with carrier OH groups, there are no visible crystals. On the other hand, the EXAFS spectra for the grafted specimens show all the oscillations found for crystalline V2O5. It is concluded that the vanadium oxide layers in these grafted materials have a long-range order similar to that in V2O5 and contain microcrystals having sizes up to 5 nm.Translated from Teoreticheskaya i Éksperimental'naya Khimiya, Vol. 23, No. 5, pp. 652–655, September–October, 1987.  相似文献   

2.
Temperature-programmed reductions (TPR) with H2 of both pure V2O5 and coprecipitated V2O5?TiO2 systems with different titanium concentrations was performed. The original and the reduced samples following each TPR step were characterized by X-ray diffraction, Fourier transform infrared analysis and scanning electron microscopy. Within the temperature range in which TPR analysis was carried out (100–600°C) the V2O5 phase was reduced in two or three steps, while no variation in the TiO2 phase (anatase or rutile) was observed. In the first reduction step only superficial reduction of the oxides was detected. In the following steps, the H2 reacted with oxygen atoms of the V=O and V?O?V bonds. This led to important changes in the structure and morphology of the system. The experimental evidence allowed the conclusion that titanium stabilizes certain phases of vanadium oxides in which vanadium appears as V(+4) or as a mixture of V(+4) and V(+5). Moreover, when moderate and high titanium concentrations were used, the reduction temperature of the bulk V2O5 decreased markedly.  相似文献   

3.
Phase equilibria in the V2O5-Ag2O system were investigated at a constant pressure of oxygen (0.2 atm) and the phase diagram found under these conditions was compared with the results of the authors who investigated the same system in vacuum and at an oxygen pressure of 1 atm. On the basis of all these results, an attempt was made to construct the hypothetical diagram of V2O5-Ag2O-O2.  相似文献   

4.
Chemical transport of the vanadium oxides V2O5, V3O7, and V6O13 The suitability of water and some halogenating transport agents (NH4Cl, NH4Br, I2) for the chemical transport (temperature gradient 850/750 K) of V2O5, V3O7, and V6O13 has been investigated. Transport rates for V2O5 and V6O13 could be measured and reproduced. The best transport agent for V2O5 is NH4Cl or H2O. For V3O7 a combination of the transport agents I2/H2O give the best results and for V6O13 the combination of NH4Br/H2O was most appropriate.  相似文献   

5.
Phase diagrams in the subsolidus area of the systems FeVO4 - CdO and FeVO4 - Cd2V2O7 have been deduced using the results of XRD and DTA analyses. On the basis of these diagrams and some additional verifying research, a projection of the subsolidus area of the CdO - V2O5 - Fe2O3 system onto the plane that comprises the components’ concentration triangle has been presented. The H-type phase is the only phase formed in this system. It co-exists at equilibrium with other phases in six subsidiary subsystems.   相似文献   

6.
Thermochemical Investigations in the System V/Nb/O. II. Chemical Transport in the Region V2O5/Nb2O5/VO2/NbO2 Transport experiments were used to support the phase relationships of the V2O5/Nb2O5/VO2/NbO2 system, which were established by annealing experiments of powder mixtures. The phase relations were studied in the NbO2-rich region of the system by means of X-ray and ESMA methods. The NbO2-rich section is characterized by the following two phase and three phase regions: Two phase region: V3Nb9O29/rutile mixed crystal V1?xNbxO2 Two phase region: BI-mixed crystal/VxNb1?xO2 Three phase region: V3Nb9O29/solubility limit LG1 (V1?xNbxO2)/BI-mixed crystal Three phase region: solubility limit LG1 (V1?xNbxO2)/BI-mixed crystal/solubility limit LG2 (VxNb1?xO2). The composition of the solubility limits LG1 and LG2 was ascertained by means of ESMA-investigation: LG1: 57.5 ± 5 mol% NbO2/43.5 ± 5 mol% VO2 LG2: 22.5 ± 5 mol% NbO2/78.5 ± 5 mol% VO2?  相似文献   

7.
Differential thermal analysis has been used for quantitative determination of heats of aluminothermic redox reaction of MnO2 and V2O5 over a wide range of temperatures. Heat of reaction V2O5?Al and MnO2?Al systems have been determined using the calibration plot established. The experimentally determined values compare well with those predicted from thermodynamic data available in the literature. It has been found that V2O5?Al system involves a higher heat of reaction in comparison to the MnO2?Al system.  相似文献   

8.
Single crystals of SnO2 and MO2 (M = Ti, Zr, Hf) oxide were grown from flux of B2O3? V2O5 system. Mixtures of the flux and the starting powder of Zn2SnO4, TiO2, ZrO2, or HfO2 were soaked at a temperature of 1030–1340°C for 10–72 hr and then were cooled down to 900°C at a rate of 5°C/hr. Grown crystals of SnO2 were pale brown needles. An increase in V2O5 content of the flux (up to V2O5/B2O3 ratio equal to 2) or in the soaking temperature increases the crystal size. A largest crystal with the size of 15.0 × 0.4 × 0.4 mm was obtained in the case of V2O5/B2O3 = 2. Crystals of TiO2 were black needles or platelets, and those of ZrO2 and HfO2 were yellowish, transparent needles or blocks. The maximum size of TiO2, ZrO2 or HfO2 crystal was 12.0 × 0.1 × 0.1 mm, 4.0 × 0.3 × 0.3 mm or 11.0 × 0.6 × 0.6 mm, respectively. The long axis of the crystals was all C-axis and main faces on the crystals were of {100} and/or {110} families. All these crystals were found to include the impurities of boron and vanadium. The electrical resistivities of SnO2 and TiO2 crystals were measured to be 1.4 × 106 and 5.6 × 104 Ω · cm at 25°C, respectively.  相似文献   

9.
The IR spectrum of V4Nb18O55 has been compared with the IR spectra of selected niobates of known structures to show structural relations between these compounds. This comparison shows that V4Nb18O55 has crystal structure related to T-Nb2O5, W16Nb18O94 and Ba2NaNb5O15. On the other hand, reaction between V2O5 and H-Nb2O5 yields a solid solution of V2O5 in VNb9O25. It has been proposed two models of synthesized solid solution with formulas V1+xNb9-xO25 or V1+xNb9O25+5x/2.Independently of Nb2O5 polymorph, used for synthesis, the metastable compound VNbO5 cannot be synthesized in the solid state below 650°C   相似文献   

10.
The vapour phase selective oxidation of 4-methylanisole to anisaldehyde was investigated over different V2O5 /MgO-Al2O3 catalysts at 673 K and normal atmospheric pressure. Among various catalysts investigated the 16 wt% V2O5 /MgO-Al2O3 catalyst provided good conversion and product selectivity. The MgO-Al2O3 mixed oxide was obtained by a co-precipitation method and V2O5 was impregnated from ammonium metavanadate. The MgO-Al2O3 support and various V2O5 /MgO-Al2O3 catalysts were characterized by means of X-ray diffraction, FT-infrared, electron spin resonance, scanning electron microscopy, ammonia and carbon dioxide chemisorption methods. The characterization results suggest that vanadia does not form layer structures on the support surface, instead interacts very strongly with the support, in particular with MgO, and forms amorphous compounds. The NH3 and CO2 uptake results provide an interesting information on the acid-base characteristics of these catalysts and correlate with their catalytic properties.  相似文献   

11.
Mixed crystals V1-xNbxO2 exist over the whole area of the quasibinary line VO2-NbO2. The existence of Nb5+ beside V3+ and V4+ on the V-rich side and V3+ beside Nb5+ and Nb4+ on the Nb-rich side of the mixed crystals is demonstrated by XANES-measurements. The compound VNbO4(V0.5Nb0.5O2) is described as a double oxide with vanadium only as V3+ and niobium only as Nb5+. At this point the electric resistivity of the solid solution shows a maximum.  相似文献   

12.
《Solid State Sciences》1999,1(5):279-286
High quality single crystals of V2Se2O9 have been obtained as a side compound during a study of the CuCl2-V2O5-SeO2 system. V2Se2O9 crystallises in the monoclinic system, space group P21/n with a = 8.0560(2), b=10.3650(2), c = 8.4500(2) Å, β = 102.893(2) °, Z = 4 and ρx =3.90 g/cm3. Full matrix least-squares refinement gave an R = 0.0347 and Rw = 0.0802 using 2232 independent reflections. The structure is built up by very distorted octahedra occupied by V5+ sharing one edge and one apex to form [V4O18]16− entities interconnected by SeO3E tetrahedra (E designs the 4s2 lone pair of the Se (IV) cation). V2Se2O9 is not isostructural with V2Te2O9, in which the V5+O6 octahedra share edges to form along [011] infinite chains linked together via Te2O5E2 groups.  相似文献   

13.
Coordination of Vanadium in the Phases 4 PbO · V2O5 and 8 PbO · V2O5 It is demonstrated, using infrared spectroscopy, that the coordination of vanadium in the two binary phases 4 PbO · V2O5 and 8 PbO · V2O5 is tetrahedral. The spectra in the V? O stretching region closely resembles that of the lead(II) orthovanadate, Pb3(VO4)2.  相似文献   

14.
Characteristic temperatures, such as T g (glass transition), T x (crystallization temperature) and T l (liquidus temperature) of glasses from the V2O5-MoO3-Bi2O3 system were determined by means of differential thermal analysis (DTA). The higher content of MoO3 improved the thermal stability of the glasses as well as the glass forming ability. The non-isothermal crystallization was investigated and following energies of the crystal growth were obtained: glass #1 (80V2O5·20Bi2O3) E G=280 kJ mol-1, glass #2 (40V2O5·30MoO3·30Bi2O3) E G=422 kJ mol-1 and glass #3 (80MoO3·10V2O5·10Bi2O3) E G=305 kJ mol-1. The crystallization mechanism of glass #1 (n=3) is bulk, of glass #3 (n=1) is surface. Bulk and surface crystallization was supposed in glass #2. The presence of high content of a vanadium oxide acts as a nucleation agent and facilitates bulk crystallization. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

15.
Mixed crystals V1-xNbxO2 exist over the whole area of the quasibinary line VO2-NbO2. The existence of Nb5+ beside V3+ and V4+ on the V-rich side and V3+ beside Nb5+ and Nb4+ on the Nb-rich side of the mixed crystals is demonstrated by XANES-measurements. The compound VNbO4(V0.5Nb0.5O2) is described as a double oxide with vanadium only as V3+ and niobium only as Nb5+. At this point the electric resistivity of the solid solution shows a maximum. Received: 11 May 1998 / Revised: 4 August 1998 / Accepted: 10 August 1998  相似文献   

16.
Differential thermal analysis (DTA) and X-ray powder diffraction (XRD) were used to study phase equilibria, established in air in the V2O5-Sb2O4 system up to 1000°C. It has been found that there is a new phase =SbVO5. The =SbVO5 has been prepared by two methods: by heating equimolar mixtures of V2O5 and α-Sb2O4 in air and by oxidation of the known phase of rutile type obtained in pure argon at temperatures between 550 and 650°C. Thermal decomposition of =SbVO5 in the solid state starts at 710°C giving off oxygen. The results provide a basis for constructing only a part of the phase diagram of the investigated system (up to 50.00 mol% Sb2O4). This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

17.
Characterization of Electrode Materials Based on V2O5 by X-Ray and Photoelectron Spectroscopy The investigation of various LixV2O5 compounds and V2O5 itself by X-ray and photoelectron spectroscopy resulted in new knowledge about the change of the structure of V2O5 during discharge in positive electrodes of secondary lithium batteries. The structures of the compounds produced by electrochemical reduction of V2O5 in aprotic lithium salt solutions are similar to these received on a chemical way. In the case of overdischarging of LixV2O5 (x > 1) the V2p3/2 binding energy is decreased, the change of the lattice becomes irreversible, and the material is after that only uncompletely rechargeable.  相似文献   

18.
Formation and Transformation of Oxide Phases in the Quasibinary System V2O5? Nb2O5 In the quasibinary system V2O5? Nb2O5 three phases exist in addition to the boundary phases: VNbO5, V2Nb9O27.5, and VNb9O25. Only the latter phase is a thermodynamically stable one. The metastable phases VNbO5 and V2Nb9O27.5 are formed by thermal decomposition of freeze-dryed products of alkoxide hydrolysis. VNb9O25 can be formed by thermal treatment of a metastable solid solution with TT-Nb2O5 structure or, beside V2O5, by thermal decomposition of the other metastable phases. A reaction scheme of formation and decomposition of phases in the quasi- binary system is given and discussed.  相似文献   

19.
Phase equilibria being established in the solid state in the system V2O5?Fe8V10W16O85 were examined by X-ray phase powder diffraction and DTA. It has been found that the system of interest is a real two-component system with an eutectic temperature 620±5°C.  相似文献   

20.
The Phase Relations in the System V/Nb/O. I. Coexistence Relations in the Section V2O5/Nb2O5/VO2/NbO2 . Phase relations in the section Nb2O5/V2O5/VO2/NbO2 of the ternary system V/Nb/O have been studied by X-ray diffraction. The investigated samples were prepared by high temperature synthesis at 900°C–1000°C. The section Nb2O5/V2O5/VO2/NbO2 is charakterized by fife three phase regions: The limits of solubility of the pseudobinary system were ascertained by determination of lattic parameters of powder samples:   相似文献   

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