纳米复合Y_2O_3/TiO_2的制备、表征及其光催化性能研究

采用溶胶 凝胶法制备复合半导体Y2 O3/TiO2 。掺入Y2 O3会阻碍锐钛矿晶相的出现 ,掺入浓度越大 ,TiO2 锐钛矿 (10 1)峰强度减小越大、平均晶粒直径与颗粒直径减小、比表面积增大 ;Y2 O3/TiO2 具有高热稳定性与高比表面积 ,由于量子尺寸效应 ,掺入Y2 O3使光催化剂的拉曼峰发生微小位移 ,在 3 80～ 460nm范围内 ,使反射率增强。以亚甲基蓝与甲基橙溶液光催化降解为模型反应 ,掺入Y2 O3,复合光催化剂对亚甲基蓝溶液的光催化脱色降解一级动力学常数明显低于纯TiO2 的 ;掺入 5 %和 10 %Y2 O3,复合光催化剂对甲基橙溶液的光催化脱色降解一级动力学均常数高于纯TiO2 的 ,掺入浓度太高反而有害。讨论了掺入Y2 O3后光物理性质的变化与其光催化活性的关系     

纳米复合Sb2O3/TiO2的光催化性能研究

采用溶胶－凝胶法制备复合纳米Sb2O3/TiO2Sb2O3掺入浓度越大,催化剂中锐钛矿相含量越高,晶粒直径与颗粒直径越小,比表面积越大,在380－460nm,范围内,Sb2O3/TiO2的反射率则减弱,表明光吸收增强,Sb^5＋,占48．42％、Sb^ 占17．58％,以亚甲基蓝溶液光催化降解为模型反应,掺入2％,5％Sb2O3,亚在蓝溶液的光催化脱色降解一致动力学常数与总有机炭（TOC）去除率增大,发射光谱证明,Sb2O3的最佳比例为2％,当其比例大于2％时,其电子空穴对的复合率升高,光催化活性下降。     

纳米复合Sb_2O_3/TiO_2的光催化性能研究

采用溶胶-凝胶法制备复合纳米 Sb2O3/TiO2。 Sb2O3掺入浓度越大,催化剂中锐钛矿相含量越高,晶粒直径与颗粒直径越小,比表面积越大。在 380～ 460nm范围内, Sb2O3/TiO2的反射率则减弱,表明光吸收增强。 XPS分析表明：掺入 2％ Sb2O3,出现新的 Ti2p3/2峰,对应于 Ti3＋,占 9.13％;锑以 Sb3＋、 Sb5＋两种形式存在, Sb5＋占 84.42％、 Sb3＋占 17.58％。以亚甲基蓝溶液光催化降解为模型反应,掺入 2％、 5％ Sb2O3,亚甲基蓝溶液的光催化脱色降解一级动力学常数与总有机炭（ TOC）去除率增大。发射光谱证明： Sb2O3的最佳比例为 2％,当其比例大于 2％时,其电子空穴对的复合率升高,光催化活性下降。     

La2O3掺杂TiO2光催化剂的制备和性能

采用溶胶-凝胶法制备了La2O3掺杂TiO2纳米光催化剂，并通过XRD、TEM、BET和XPS等手段进行了表征．掺入La2O3后，阻止了TiO2从锐钛矿晶型向金红石晶型的转变，使TiO2的粒径减小，比表面积增大．以甲基橙为光催化降解反应模型化合物，考察了光催化剂的活性．测定了甲基橙在纯TiO2和La2O3掺杂TiO2光催化剂上的吸附常数．考察了pH、H2O2对降解性能的影响．讨论了光催化活性与催化剂性质的关系．     

WO3/TiO2纳米材料的制备及光催化性能

采用溶胶-凝胶法制备WO3/TiO2复合纳米光催化剂,掺入WO3、TiO2锐钛矿101峰的相对强度、平均晶粒直径与颗粒直径均减小,比表面积增大;WO3掺入摩尔比分别为2%、5%、8%时,新的LRS峰位分别出现在797、967及969cm-1;在380-460nm范围内,WO3/TiO2的反射率减小,XPS分析表明,WO3/TiO2晶体中存在W6+、W5+、W4+、和Ti4+、Ti3+。以亚甲基兰的光催化降解为反应模型,掺入WO3后,光催化活性增强,掺入摩尔比为2%时,WO3/TiO2的光催化活性最高。还讨论了光催化活性与性质的关系。     

活性炭负载TiO2-Fe3O4磁性光催化剂的制备及性能

采用溶胶-凝胶法制备了易于固液分离的活性炭（AC）负载磁性光催化剂（TiO2-Fe3O4／AC）．样品通过SEM-EDX和X射线衍射法进行表征．通过在紫外光照射下降解亚甲基蓝评价其光催化降解能力．结果表明：负载22％Fe3O4的光催化剂（含20％TiO2和58％AC）的光催化活性最强（120min时亚甲基蓝的降解率达到87％,是纯TiO2的2．7倍）;磁性光催化剂可实现磁分离回收．     

超声微乳法合成TiO2-SiO2催化剂可见光光催化降解亚甲基蓝

采用可见光下亚甲基蓝的光催化降解为模型反应,考察了超声微乳法经钛酸丁酯水解合成的纳米TiO2-SiO2催化剂的性能,并用XRD和BET对催化剂进行了表征。结果表明:硅胶的加入有效地提高了TiO2-SiO2催化剂的热稳定性,抑制了热处理过程中TiO2由锐钛矿相向金红石相的转变和晶粒的长大。随着焙烧温度和TiO2含量的增加,TiO2的晶粒变大,但比表面积减少。TiO2-SiO2的光催化活性明显改善,可见光照射120min,31%TiO2/SiO2催化剂存在下,有84%亚甲基蓝光催化降解。31%TiO2/SiO2催化剂光降解亚甲基蓝的能力大大优于Degussa P-25和纯TiO2,其降解亚甲基蓝的反应速率常数分别为P-25和纯TiO2的8倍和10倍。     

磁性TiO2/CoFe2O4纳米复合光催化材料的制备

以磁性CoFe2O4为核,采用改进的溶胶-凝胶法,制备了磁性TiO2/CoFe2O4纳米复合光催化材料.利用VSM(振动样品磁强计)技术对其磁性能进行了研究,结果表明:由该法所得的TiO2/CoFe2O4纳米复合光催化材料的饱和磁化强度虽稍弱于纯CoFe2O4纳米材料,但其矫顽力则优于CoFe2O4.TEM、XRD、UV-Vis等的结果表明,该纳米复合材料中的TiO2为锐钛矿结构;与TiO2相比,纳米复合材料对光的吸收拓展到了整个紫外-可见区,且吸收强度大大增强.对染料废水光催化降解的模拟研究表明,该复合材料在紫外光下,6 h可以使亚甲基蓝染料溶液的脱色率达95%,且重复使用3次时染料溶液的脱色率仍能保持在90%,明显优于纯TiO2.     

Eu3＋、Si4＋共掺杂TiO2光催化剂的协同效应

采用溶胶-凝胶-浸渍法制备了Eu/Ti/Si纳米光催化剂, 并通过XRD、FT-IR、EPR等进行了表征.结果表明,掺入Eu3＋和Si4＋, 阻止了TiO2从锐钛矿晶型向金红石晶型的转变, 使TiO2的粒径减小, 且Eu3＋能够促进Si4＋进入TiO2的晶格中.以甲基橙为光催化反应模型化合物, 考察了光催化剂的活性.测定了甲基橙在不同光催化剂上的吸附常数,探讨了催化剂对甲基橙的吸附机理. Eu3＋和Si4＋的最佳掺入量分别为wEu=0.03％、wSiO2=39.06％,且Eu3＋和Si4＋同时掺入TiO2光催化剂产生协同效应.讨论了光催化活性与催化剂性质的关系.     

Eu~(3 )、Si~(4 )共掺杂TiO_2光催化剂的协同效应

采用溶胶-凝胶-浸渍法制备了Eu/Ti/Si纳米光催化剂,并通过XRD、FT-IR、EPR等进行了表征.结果表明,掺入Eu3 和Si4 ,阻止了TiO2从锐钛矿晶型向金红石晶型的转变,使TiO2的粒径减小,且Eu3 能够促进Si4 进入TiO2的晶格中.以甲基橙为光催化反应模型化合物,考察了光催化剂的活性.测定了甲基橙在不同光催化剂上的吸附常数,探讨了催化剂对甲基橙的吸附机理.Eu3 和Si4 的最佳掺入量分别为wEu=0.03%、wSiO2=39.06%,且Eu3 和Si4 同时掺入TiO2光催化剂产生协同效应.讨论了光催化活性与催化剂性质的关系.     

Intermolecular forces for D2, N2, O2, F2 and CO2

The intermolecular potentials for D₂, N₂, O₂, F₂ and CO₂ are determined on the basis of the second virial coeffincients, the polarizabilities parallel and perpendicular to the molecular axes, and the electric quadrupole moment. The repulsive parts of the potentials are taken from the corresponding Kihara core-potentials. Effects of the octopolar induction are taken into consideration in a unique way. The potential depends on relative orientations of the two molecules as well as the distance r between the molecular centers. This dependence is shown in graphs. A measure of the anisotropy of the potential depth is 0.72 for CO₂ 0.36 for D₂, and smaller than 0.27 for N₂ O₂ and F₂. The remarkable anisotropy for CO₂ and D₂ is due to strong electrostatic quadrupole interactions.     

Ba3 (VO4)2-K2 Ba(MoO4)2 and Pb3 (VO4)2-K2 Pb(MoO4)2 systems

Phase equilibria in the Ba₃(VO₄)₂-K₂Ba(MoO₄)₂ and Pb3(VO₄)₂-K₂Pb(MoO₄)₂ systems have been investigated. In the first system, a continuous series of substitutional solid solutions with the palmierite structure is formed, and in the second one, the polymorphic transition in lead orthovanadate at 100°C restricts the extent of the palmierite-type solid solution to 10–100 mol % K₂Pb(MoO₄)₂. Original Russian Text ? V.D. Zhuravlev, Yu.A. Velikodnyi, A.S. Vinogradova-Zhabrova, A.P. Tyutyunnik, V.G. Zubkov, 2008, published in Zhurnal Neorganicheskoi Khimii, 2008, Vol. 53, No. 10, pp. 1746–1748.     

配合物[Cu(H2O)(C12H8N2)2].2ClO4的合成、性质及晶体结构

合成了配合物[Cu(H2O)(C12H8N2)2]*2ClO4(C12H8N2为1,10-邻菲咯啉),用元素分析、摩尔电导、红外光谱及电子光谱进行了表征,并测定了配合物的晶体结构.该晶体属单斜晶系,空间群为CC;晶胞参数a=1.9177(2)nm,b=0.81994(0)nm,c=1.62458(14)nm,β=100.104(6)°;V=2.5419(4)nm3,Z=4,F(000)=1300,DC=1.693g/cm3,R=0.0430,wR=0.1195.中心铜(Ⅱ)离子与两个1,10-邻菲咯啉的四个N原子和一个水分子的氧原子配位,形成了一个变形的三角双锥结构.     

The preparation of NbH5(Me2PCH2CH2Me2)2 and NbHL2(Me2PCH2CH2PMe2)2 (L = CO or C2H4)

MMe₅(dmpe) (M = Nb or Ta, dmpe = Me₂PCH₂CH₂PMe₂) reacts with H₂ (500 atm) and dmpe in THF at 60°C to give MH₅(dmpe)_2? NbH₅(dmpe)₂ readily reacts with two mol of CO or ethylene (L) to give NbHL₂(dmpe)₂. The exchange of the hydride ligand with the ethylene protons in NbH(C₂H₄)₂(dmpe)₂ is not rapid on the ¹H NMR time scale (60 MHz) at 95°C.     

Phase transitions in Ca3(BN2)2 and Sr3(BN2)2

α-Ca₃(BN₂)₂ crystallizes in the cubic system (space group: ) with one type of calcium ions disordered over of equivalent (8c) positions. An ordered low-temperature phase (β-Ca₃(BN₂)₂) was prepared and found to crystallize in the orthorhombic system (space group: Cmca) with lattice parameters: , , and . Structure refinements on the basis of X-ray powder data have revealed that orthorhombic β-Ca₃(BN₂)₂ corresponds to an ordered super-structure of cubic α-Ca₃(BN₂)₂. The space group Cmca assigned for β-Ca₃(BN₂)₂ is derived from by a group-subgroup relationship.DSC measurements and temperature-dependent in situ X-ray powder diffraction studies showed reversible phase transitions between β- and α-Ca₃(BN₂)₂ with transition temperatures between 215 and 240 °C.The structure Sr₃(BN₂)₂ was reported isotypic with α-Ca₃(BN₂)₂ () with one type of strontium ions being disordered over of equivalent (2c) positions. In addition, a primitive () structure has been reported for Sr₃(BN₂)₂. Phase stability studies on Sr₃(BN₂)₂ revealed a phase transition between a primitive and a body-centred lattice around 820 °C. The experiments showed that both previously published structures are correct and can be assigned as α-Sr₃(BN₂)₂ (, high-temperature phase), and β-Sr₃(BN₂)₂ (, low-temperature phase).A comparison of Ca₃(BN₂)₂ and Sr₃(BN₂)₂ phases reveals that the different types of cation disordering present in both of the cubic α-phases () have a directing influence on the formation of two distinct (orthorhombic and cubic) low-temperature phases.     

Zur Trennung von H2, O2, N2, NO, CO, N2O, CO2, C2H6, C2H4, C2H2, NO2(N2O4) und Feuchtigkeit

Ohne Zusammenfassung     

Conversion of NO in NO/N2, NO/O2/N2, NO/C2H4/N2 and NO/C2H4/O2/N2 Systems by Dielectric Barrier Discharge Plasmas

An experimental study on the conversion of NO in the NO/N₂, NO/O₂/N₂, NO/C₂H₄/N₂ and NO/C₂H₄/O₂/N₂ systems has been carried out using dielectric barrier discharge (DBD) plasmas at atmospheric pressure. In the NO/N₂ system, NO decomposition to N₂ and O₂ is the dominating reaction; NO conversion to NO₂ is less significant. O₂ produced from NO decomposition was detected by an on-line mass spectrometer. With the increase of NO initial concentration, the concentration of O₂ produced decreases at 298 K, but slightly increases at 523 K. In the NO/O₂/N₂ system, NO is mainly oxidized to NO₂, but NO conversion becomes very low at 523 K and over 1.6% of O₂. In the NO/C₂H₄/N₂ system, NO is reduced to N₂ with about the same NO conversion as that in the NO/N₂ system but without NO₂ formation. In the NO/C₂H₄/O₂/N₂ system, the oxidation of NO to NO₂ is dramatically promoted. At 523 K, with the increase of the energy density, NO conversion increases rapidly first, and then almost stabilizes at 93–91% of NO conversion with 61–55% of NO₂ selectivity in the energy density range of 317–550 J L⁻¹. It finally decreases gradually at high energy density. A negligible amount of N₂O is formed in the above four systems. Of the four systems studied, NO conversion and NO₂ selectivity of the NO/C₂H₄/O₂/N₂ system are the highest, and NO/O₂/C₂H₄/N₂ system has the lowest electrical energy consumption per NO molecule converted.     

Formation of [Cp2TiSbMe2]2, [Cp2TiSb(SiMe3)2]2 and [Cp2TiCl]2·2Mes4Sb2

Reactions of [Cp₂Ti(btmsa)] (btmsa = bis(trimethylsilyl)acetylene) with R₄Sb₂ (R = Me, Me₃Si) give [Cp₂TiSbMe₂]₂ (1) or [Cp₂TiSb(SiMe₃)₂]₂ (2) respectively. [Cp₂TiCl]₂·2Mes₄Sb₂ (3) is serendipitously formed from [Cp₂Ti(btmsa)] and Mes₂SbH containing NH₄Cl traces.     

Synthesis and structural investigation of the compounds containing HF2 anions: Ca(HF2)2, Ba4F4(HF2)(PF6)3 and Pb2F2(HF2)(PF6)

Three new compounds Ca(HF₂)₂, Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) were obtained in the system metal(II) fluoride and anhydrous HF (aHF) acidified with excessive PF₅. The obtained polymeric solids are slightly soluble in aHF and they crystallize out of their aHF solutions. Ca(HF₂)₂ was prepared by simply dissolving CaF₂ in a neutral aHF. It represents the second known compound with homoleptic HF environment of the central atom besides Ba(H₃F₄)₂. The compounds Ba₄F₄(HF₂)(PF₆)₃ and Pb₂F₂(HF₂)(PF₆) represent two additional examples of the formation of a polymeric zigzag ladder or ribbon composed of metal cation and fluoride anion (MF⁺)_n besides PbF(AsF₆), the first isolated compound with such zigzag ladder. The obtained new compounds were characterized by X-ray single crystal diffraction method and partly by Raman spectroscopy. Ba₄F₄(HF₂)(PF₆)₃ crystallizes in a triclinic space group P1¯ with a=4.5870(2) Å, b=8.8327(3) Å, c=11.2489(3) Å, α=67.758(9)°, β=84.722(12), γ=78.283(12)°, V=413.00(3) Å³ at 200 K, Z=1 and R=0.0588. Pb₂F₂(HF₂)(PF₆) at 200 K: space group P1¯, a=4.5722(19) Å, b=4.763(2) Å, c=8.818(4) Å, α=86.967(10)°, β=76.774(10)°, γ=83.230(12)°, V=185.55(14) ų, Z=1 and R=0.0937. Pb₂F₂(HF₂)(PF₆) at 293 K: space group P1¯, a=4.586(2) Å, b=4.781(3) Å, c=8.831(5) Å, α=87.106(13)°, β=76.830(13)°, γ=83.531(11)°, V=187.27(18) Å³, Z=1 and R=0.072. Ca(HF₂)₂ crystallizes in an orthorhombic Fddd space group with a=5.5709(6) Å, b=10.1111(9) Å, c=10.5945(10) Å, V=596.77(10) Å³ at 200 K, Z=8 and R=0.028.     

Vapour-liquid equilibrium data for the systems C2H6 + N2, C2H4 + N2, C3H8 + N2, and C3H6 + N2

High pressure vapour-liquid equilibrium data for the C₂H₆ + N₂, C₂H₄ + N₂, C₃H₈ + N₂, and C₃H₆ + N₂ systems are presented. The data are obtained isothermally in the range from 200 K to 290 K. For each point of data, temperature, pressure and liquid and vapour phase mole fractions are measured.Values for the vapour phase mole fractions are calculated from the obtained pressure, temperature and liquid phase mole fractions. The calculated values are compared with the experimental results, and it is found that the average mean deviation between calculated and experimental mole fractions is less than 0.009 for the systems considered in this work.