纳米颗粒的超临界干燥法制备及用于醋酸乙烯蒸气的催化发光检测

利用乙醇超临界流体干燥技术 (SCFD)(280 ℃× 7.0 MPa×30 min)制备了纳米MgO及Y2O3颗粒,发现其对一些有害气体的催化发光强度远高于普通干燥技术制备的纳米MgO及Y2O3.设计了一种以SCFD技术合成的纳米MgO为敏感材料,催化发光检测醋酸乙烯蒸气的传感器.此传感器具有很高的灵敏度及优异的选择性,在温度279 ℃、波长425 nm、空气流速为160 mL/min的最佳条件下,催化发光强度与醋酸乙烯蒸气浓度在1.8～1800 mg/m3内呈良好的线性关系,检出限为0.7 mg/m3.当浓度相同的丙酮、乙醛、乙酸乙酯、乙酸、甲醛、氨水、乙醇、苯和甲醇蒸气通过此传感器时,除乙醇引起3.56%的干扰外,其它气体基本不干扰醋酸乙烯的测定.应用本方法可快速测定车间空气中的醋酸乙烯.     

一种高选择性的检测丙酮蒸气催化发光传感器

设计了一种基于纳米材料SrCO3中掺杂Dy2O3的催化发光(CTL)丙酮蒸气传感器。通过掺杂Dy2O3使体系选择性显著提高。当Dy2O3的掺杂量为33%时,催化发光强度是不掺杂的3倍。当各测试气体浓度均为2000mL/m3时,三氯甲烷、二氯乙烷、甲醛和苯气体不干扰丙酮的测定。乙醇和正丁烷只引起15%和2.1%的干扰。在温度383℃、波长425nm、空气流速为360mL/min的最佳条件下,催化发光强度与丙酮蒸气浓度在1.0～5000mL/m3内呈良好的线性关系,检出限为0.30mL/m3。本传感器响应和恢复时间快速。     

基于四氧化三钴材料催化发光的丙醛气体传感器研究

研究发现, 在一定条件下丙醛气体在四氧化三钴材料表面上具有催化发光特性,基于此建立了一种检测空气中痕量丙醛气体的催化发光传感器.在对合成的3种形貌四氧化三钴的催化发光性质进行比较的基础之上,对分析方法条件进行了优化,其结果表明:在以微球状四氧化三钴作为传感材料,检测波长490 nm, 反应温度232 ℃,载气流速400 mL/min的最优条件下,可测定的丙醛气体浓度的线性范围为0.3～171 mg/L(r=0.9977, n=13),检出限为0.1 mg/L(S/N=3),测定4.8 mg/L丙醛的相对标准偏差为1.8%(n=5).此外,考察了相同浓度的常见挥发性有机物的干扰情况,其结果表明该传感器具有很好的选择性.连续80 h通过4.8 mg/L丙醛,发光强度无明显降低,相对标准偏差小于5%,表明此传感器使用寿命长.并将该传感器成功用于人工合成样品的分析,回收率在91%～103%之间,测定浓度值与实际组成基本相符.     

基于硼酸镝催化发光法的正丙醇气体传感器的研究

基于正丙醇在硼酸镝材料表面有强烈的发光现象,设计了以硼酸镝为传感材料检测正丙醇的传感器。该传感器在波长为535 nm、温度为150℃、载气流速为200 m L/min时,测定正丙醇质量浓度工作曲线的线性范围为40~1800 mg/m~3(R=0.9955),检出限为15 mg/m~3。选择了13种干扰气体(丙酮、二甲苯、正己烷、三氯化碳、丙醛、乙醛、四氯化碳、苯、异丙醇、二氯化碳、甲醇、乙醇、正丁醇)进行选择性测试,除二氯化碳、乙醇、正丁醇分别有4%,9%,5%左右的干扰外,其他气体并无干扰。连续通入45 h 300 mg/m~3的正丙醇,发光强度无明显变化,传感器具有良好的使用寿命。     

提取多维催化发光信号鉴别有害气体的传感器

基于2种催化敏感材料, 设计了通过提取多维发光信号鉴别有害气体的催化发光(CTL)传感器. 在最佳检测条件下, 18种有害气体依次经过纳米Al₂O₃(或MgO)表面进行CTL反应, 产生的CTL 响应信号组成其特征图谱. 通过主成分分析法(PCA)鉴别了各种气体. 采用线性判别分析(LDA)对浓度分别为100, 300及500 mL/m³的18种气体的识别正确率均为100%. 该传感器可以同时测量气体的浓度, 检出限均低于我国工作场所有害因素职业接触限值(GBZ2.1-2007), 空气中几种常见的污染物共存不影响这些有害气体的检测. 该传感器具有传感元件少、 稳定性好、 操作方便、 信息丰富和识别能力强等优点, 可用于发展微型实用的传感器.     

检测易爆气体的催化发光传感器研究

报道了一种用于定量分析易爆气体混合物丙烷和异丁烷的基于碳酸锶纳米材料的催化发光传感器.基于该传感器在不同温度下对两种气体的灵敏度不同,在320℃和342℃两个工作温度下,两种气体的浓度范围均为1000 mL/m3～10000 mL/m3时,分别建立了混合组分浓度相对催化发光强度的两个线性回归方程.在342℃时,丙烷和异丁烷的检出限(3σ)分别为50 mL/m3和20 mL/m3.可通过解上述两个联立方程式求得未知混合物中两组分的浓度.外来物质甲烷、乙烷、CO、氨气通过传感器时,甲烷和乙烷分别引起5.6%和17.2%的干扰,其它气体不干扰测定.20000 mL/m3的水蒸气不干扰2000 mL/m3丙烷和异丁烷气体的测定.用该法分析了人工合成样品中两种气体的浓度.     

基于纳米复合氧化物催化发光的乙醇传感器

基于纳米材料上乙醇的催化发光现象,建立了直接测定空气中乙醇浓度的方法.实验发现,乙醇在纳米级钛锆镧(原子比为5∶2∶1)复合氧化物表面有较高的发光强度和较好的选择性,以此为敏感材料可以建立一种高效稳定的乙醇气体传感器,其最佳操作条件为:分析波长620nm,测定温度310℃,载气流速130mL/min.方法的检测限为(3σ)1.3mg/m3,线性范围为2～230mg/m3,相关系数为0.9990,回收率为97.4%～102.7%.对常见共存物的研究发现,甲醛、丙酮、苯、氨、二氧化硫和二氧化碳都不干扰测定,该传感器的连续工作时间可达120h以上.     

基于纳米ZnO-ZrO2催化发光丙酮传感器的研究

研究了丙酮在纳米ZnO-ZrO2(质量比为4:1)表面催化发光行为,发现基于这种纳米催化剂的气体传感器对丙酮的检测具有高灵敏度和较强的选择性。在波长460 nm,温度219℃,载气流速25 mL/min时进行定量分析,催化发光强度与丙酮浓度在一定范围内呈良好的线性关系,线性范围为0.1～4000 mL/m3(r=0.9996,n=6);检出限为1.6 mL/m3(S/N=3)。传感器工作时间可达106h以上,可用于丙酮的实时在线检测。     

复合ZrO2/MgO催化发光丙烯醛气体传感器

设计了基于在纳米ZrO2中掺杂Mg0的催化发光传感器,以快速检测丙烯醛气体.与纯ZrO2相比,MgO的掺杂量为5%时,丙烯醛的催化发光强度增大了1.8倍,干扰气体乙醛的催化发光强度降为原来的约1/7.传感器在波长425 nm,温度279 ℃,流速200 mL/min条件下,对丙烯醛具有高灵敏度和选择性,发光强度与丙烯醛...     

基于CeO2-Co3O4纳米纤维的催化发光式甲醛传感器研究

采用双喷嘴静电纺丝法制备了CeO2-Co3 O4纳米纤维,将制备的CeO2-Co3 O4纳米纤维均匀涂覆于 ω型加热线圈表面形成催化发光薄膜,设计了一种新型催化发光甲醛传感器.采用X射线衍射仪、 扫描电子显微镜、 全自动程序化学吸附仪和X-射线光电子能谱仪,表征了Co3 O4-CeO2纳米纤维的相组成和微观形貌,讨论了甲醛在CeO2-Co3 O4催化剂表面的电化学特性和催化发光机理.在优化条件下,即波长500 nm、 温度550℃ 、 载气流速0.2 L/min,甲醛传感器件(Ce30)催化发光强度与甲醛浓度在1.2~50μg/m3范围内有良好的线性关系,灵敏度为40.04 a.u./(μg/m3),检出限为1.2μg/m3,动态响应和恢复时间分别为2.4和3.5 s.此传感器可用于汽车尾气中甲醛浓度检测,相对误差范围为0.4%~1.1%,相对标准偏差RSD<3%(n=6).     

KCl-KBO2-K2CO3, K2MoO4-KBO2-K2CO3, and K2WO4-KBO2-K2CO3 ternary systems

phase diagrams of KCl-KBO₂-K₂CO₃, K₂MoO₄-KBO₂-K₂CO₃, and K₂WO₄-KBO₂-K₂CO₃ ternary systems were studied by a calculation-experimental method and differential thermal analysis (DTA). The coordinates of ternary eutectics were determined to be E ₁: 622°C, 8.5 mol % KBO₂, 56.5 mol % KCl, and 35 mol % K₂CO₃; E ₂: 710°C, 23 mol % KBO₂, 43 mol % K₂CO₃, and 34 mol % K₂MoO₄; E ₃: 710°C, 23 mol % KBO₂, 43 mol % K₂CO₃, and 34 mol % K₂WO₄. The specific heats of melting of the eutectics were determined.     

Phase relations in the K2W2O7-K2WO4-KPO3-Bi2O3 system and structure of K6.5Bi2.5W4P6O34

The phase relations in the cross-section of the K₂W₂O₇-K₂WO₄-KPO₃ containing 15 mol% Bi₂O₃ were undertaken using flux method. Crystallization fields of K_6.5Bi_2.5W₄P₆O₃₄, K₂Bi(PO₄)(WO₄), Bi₂WO₆, KBi(WO₄)₂ and their cocrystallization areas were identified. Novel phase K_6.5Bi_2.5W₄P₆O₃₄ was characterized by single-crystal X-ray diffraction: sp. gr. P−1, a=9.4170(5), b=9.7166(4), c=17.6050(7) Å, α=90.052(5)°, β=103.880(5)° and γ=90.125(5)°. It has a layered structure, which contains {K₇Bi₅W₈P₁₂O₆₈}_∞ layers stacked parallel to ab plane and sheets composed by potassium atoms separating these layers. Sandwich-like {K₇Bi₅W₈P₁₂O₆₈}_∞ layers are assembled from [W₂P₂O₁₃]_∞ and [BiPO₄]_∞ building units, and are penetrated by tunnels with K/Bi atoms inside. FTIR-spectra of K₂Bi(PO₄)(WO₄) and K_6.5Bi_2.5W₄P₆O₃₄ were discussed on the basis of factor group theory.     

Sol-gel synthesis of K3InF6 and structural characterization of K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18

K₃InF₆ is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K₂InC₁₀O₁₀H₆F₉, K₃InC₁₂O₁₄H₄F₁₈ and K₃InC₁₂O₁₂F₁₈. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K₃InF₆ by decomposition at high temperature. The crystal structure of K₃InC₁₂O₁₄H₄F₁₈ is characterized by complex anions [In(CF₃COO)₄(OH_x)₂]^(5−2x)− and isolated [CF₃COOH_2−x]^(x−1)− molecules with x=2 or 1, surrounded by K⁺ cations. The crystal structure of K₃InC₁₂O₁₂F₁₈ is only constituted by complex anions [In(CF₃COO)₆]³⁻ and K⁺ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K₂InC₁₀O₁₀H₆F₉ and K₃InC₁₂O₁₂F₁₈ were also performed at room temperature on pulverized crystals.     

Solubility in the Na2Cr2O7-(NH4)2Cr2O7-K2Cr2O7-H2O system

Solubility in the Na₂Cr₂O₇-(NH₄)₂Cr₂O₇-K₂Cr₂O₇-H₂O four-component water-salt system at 25, 50, and 75°C was studied for the first time. Phase field boundaries for individual salts and potassium and ammonium dichromate solid solutions, monovariant lines, and invariant points were determined. Experimental data were used to optimize the looped isohydric process of potassium dichromate preparation involving additional salts.     

NaBO2-NaCl-Na2CO3, NaBO2- Na2CO3-NaMoO4, NaBO2- Na2CO3-NaWO4, and NaBO2-NaCl-Na2WO4 ternary systems

The phase diagrams of the NaBO₂-NaCl-Na₂CO₃, NaBO₂-Na₂CO₃-Na₂MoO₄, NaBO₂- Na₂CO₃-Na₂WO₄, and NaBO₂-NaCl-Na₂WO₄ ternary systems were studied by a calculation-experimental method and differential thermal analysis. The coordinates of ternary eutectics were determined: E ₁: 612°C, 16 mol % NaBO₂, 42 mol % NaCl, and 42 mol % Na₂CO₃; E ₂: 568°C, 12 mol % NaBO₂, 28 mol % Na₂CO₃, and 60 mol % Na₂MoO₄; E ₃: 575°C, 12 mol % NaBO₂, 32 mol % Na₂CO₃, and 56 mol % Na₂WO₄; E ₄: 628°C, 8 mol % NaBO₂, 20 mol % NaCl, and 72 mol % Na₂WO₄; and E ₅: 655°C, 9 mol % NaBO₂, 53 mol % NaCl, and 38 mol % Na₂WO₄.     

Li2SO4-Na2SO4-H2O和Li2SO4- K2SO4-H2O溶液的体积性质

本文用高精度数字式振荡管密度计测定了288K至318K温度范围内Li₂SO₄ + Na₂SO₄ + H₂O和 Li₂SO₄ + K₂SO₄ + H₂O三元体系的密度。混合溶液的离子强度范围从0.1到4.5 mol.kg_–1,混合溶液中Na₂SO₄和K₂SO₄的离子强度分数为0.2,0.4,0.6和0.8。用密度实验值拟合得到了不同温度下Pitzer离子相互作用模型混合参数θ_V和 ψ_V,模型的计算值与实验值的偏差在±0.002 g.cm_–3以内。用Pitzer模型计算了不同离子强度下三元体系的混合体积。     

Extension of the La7Mo7O30 structural type with La7Nb3W4O30 and La7Ta3W4O30 compounds

Two compounds of formula La₇A₃W₄O₃₀ (with A=Nb and Ta) were prepared by solid-state reaction at 1450 and 1490 °C. They crystallize in the rhombohedric space group R-3 (No. 148), with the hexagonal parameters: , and , . The structure of the materials was analyzed from X-ray, neutron and electronic diffraction. These oxides are isostructural of the reduced molybdenum compound La₇Mo₇O₃₀, which are formed of perovskite rod along [111]. An order between (Nb, Ta) and W is observed.     

SnSbBiS4-SnS and SnSbBiS4-Sn2Sb6S11 sections of the SnS-Sb2S3-Bi2S3 ternary system

SnSbBiS₄-SnS and SnSbBiS₄-Sn₂Sb₆S₁₁ sections were studied by physicochemical methods (DTA, X-ray powder diffraction, microstructure observation, and microhardness measurements). These sections were found to be eutectic quasi-binary sections of the SnS-Sb₂S₃-Bi₂S₃ ternary system. Solid solution regions based on the initial components were found on either side of the sections. Alloys in the solid solution region are p-type semiconductors.     

Theoretical study of polyoxide clusters B20O30, Al20O30, V20O50, Si20O30H20, and Si20O30F20

The structural, electronic, and vibrational characteristics and energies of the isolated polyoxide clusters B₂₀O₃₀, Al₂₀O₃₀, V₂₀O₅₀, Si₂₀O₃₀H₂₀, and Si₂₀O₃₀F₂₀ and their complexes with the H⁻ ion and ammonia complexes Al₂₀O₃₀ · nNH₃ have been calculated by the density functional theory B3LYP method with different basis sets. The computation results show that the symmetric closo structure I _h with oxygen bridges located above the centers of the faces of an empty [M₂₀] dodecahedron is more favorable for V₂₀O₅₀, Si₂₀O₃₀H₂₀, and Si₂₀O₃₀F₂₀. For B₂₀O₃₀, the cage closo isomer is also more favorable than the other isomers, but its structure is severely distorted as compared to a dodecahedron and has a symmetry close to C ₃ . For Al₂₀O₃₀, the I _h structure corresponds to a high-lying local minimum of the potential energy surface. For Al₂₀O₃₀, a set of unusual puckshaped isomers of symmetry C _i , with different numbers of four-coordinate atoms ^IVAl and three-coordinate atoms ^IIIO, was localized; these structures are more than 90 kcal/mol more favorable than the dodecahedron I _h . The most favorable isomer of Al₂₀O₃₀ contains twelve four-coordinate atoms ^IVAl and four five-coordinate atoms ^VAl. The energies of dissociation of the most favorable M₂₀O₃₀ clusters into the M₂O₃ (C _2v ) and M₄O₆ (T _d ) fragments and, in the case of Al₂₀O₃₀, also into the Al₈O₁₂ (O _h ) and Al₁₂O₁₈ (D _3d ) fragments, have been estimated. The conclusion has been drawn that these clusters can, in principle, exist and can be experimentally detected in the isolated state. Analogous calculations have been performed for ammonia complexes Al₂₀O₃₀ · nNH₃ with n varying from 1 to 20. The effect of solvation on the relative stability of the dodecahedral and puckshaped isomers of the Al₂₀O₃₀ cluster is observed. The isomers with ammonia molecules in their first coordination sphere become much closer to one another on the energy scale; however, the dodecahedron remains a considerably less favorable intermediate. Original Russian Text ? O.P. Charkin, N.M. Klimenko, D.O. Charkin, 2008, published in Zhurnal Neorganicheskoi Khimii, 2008, Vol. 53, No. 4, pp. 624–635.     

Structural chemistry of Sr3Cr2WO9, Ca3Cr2WO9, and Ba3Cr2WO9

We have studied the preparation and crystallographic structure of three perovskite-type compounds: Sr₃Cr₂WO₉, cubic, the lattice parameter of which is a = 7.812Å; Ca₃Cr₂WO₉, tetragonal, the lattice parameters of which are a = 5.408 Å and c = 7.635Å; and Ba₃Cr₂WO₉, hexagonal, the lattice parameters of which are a = 5.691 Å and c = 13.957Å. We have compared these three structures and shown the relationship between the dimensions of the alkaline-earth metal and the existence of the different structures.