正、反向共沉淀法对Pr2Zr2O7纳米粒子表观活化能的影响

以氨水作为沉淀剂,采用正、反向共沉淀法制备Pr₂Zr₂O₇纳米粒子。利用XRD、SEM、TEM、TG-DTA等测试手段表征了样品物相及形貌;研究其制备过程中合成动力学和晶粒生长动力学,采用Doyle-Ozawa法和Kissinger法分别计算正、反向沉淀粒子在主要反应阶段的表观活化能。结果表明：反向沉淀的滴定速率为2mL·min^-1、母盐溶液初始浓度0.05mol·L^-1、反应体系温度273K、pH值11、煅烧温度为1173K,保温2h的条件下获得的样品形貌近球形、无团聚现象、一次粒径约60nm。Pr₂Zr₂O₇前驱体的分解过程分为3个阶段,正、反向粒子各阶段平均表观活化能分别为：71.2、197.8、183.2kJ·mol^-1和45.37、84.34、152.16kJ·mol^-1;晶粒生长活化能分别为19.02和11.95kJ·mol^-1,后者比前者的晶粒生长活化能降低了7.07kJ·mol^-1;反向共沉淀制备工艺优于正向共沉淀法。     

煤炭燃烧过程中N2O消除反应机理的密度泛函理论研究

用密度泛函理论B3LYP方法对煤炭燃烧过程中N₂O的消除反应进行研究。选用6-311++G**和aug-cc-pVTZ基组,优化了反应通道上反应物、过渡态和产物的几何构型。预测了它们的热力学性质(总能量、焓、熵和吉布斯自由能)及其随温度的变化。预测N₂O+CO反应的活化能为200 kJ·mol^-1,与实验值193±8 kJ·mol^-1较一致。计算了500~1 800 K 温度范围的反应速率常数。在N₂O的分解中,N₂O与H和CN自由基的反应为动力学优先进行的反应,其活化能为50~55 kJ·mol^-1。在B3LYP/aug-cc-pVTZ level水平下,N₂O+CN反应是热力学最有利的自发反应,其吉布斯自由能变化为-407 kJ·mol^-1。     

静电纺丝法制备La2CuO4纳米管阴极材料及其电化学性质研究

采用静电纺丝法制备了一维管状中温固体氧化物燃料电池(ITSOFC)阴极材料La₂CuO₄。利用XRD、TG-DTA、FT-IR和SEM对材料的结构和微观形貌进行分析。研究表明,700℃烧结2h得到平均直径150纳米、形貌均一的La₂CuO₄纳米管。900℃烧结0.5h得到纳米管间连接充分并与电解质紧密接触的纤维电极。利用交流阻抗技术对电极的性能进行研究发现,La₂CuO₄纳米管阴极材料具有比粉体材料更优越的电极性能。纳米管阴极在700℃的极化电阻为1.03Ω·cm²,而同一组成粉体电极的极化电阻为1.61Ω·cm²;氧分压测试结果显示纳米管电极反应的速率控制步骤为电荷转移过程。     

纳米结晶体Ni0.5Zn0.5Fe2O4对高氯酸铵热行为及分解反应动力学的影响

采用差示扫描量热法(DSC)、热重和微分热重(TG-DTG)及固相原位反应池/快速扫描傅立叶变换红外联用技术(hyphenated in situ thermolysis/RSFTIR)研究了纳米结晶体Ni_0.5Zn_0.5Fe₂O₄与高氯酸铵(AP)组成的混合物的热行为和分解反应动力学。结果表明：Ni_0.5Zn_0.5Fe₂O₄使得AP的低、高温分解放热峰温分别提前17.44 K和27.74 K,并使得对应的分解热分别增加3.7 J·g^-1和193.7 J·g^-1。Ni_0.5Zn_0.5Fe₂O₄并不影响AP的晶转温度和晶转热。Ni_0.5Zn_0.5Fe₂O₄使得AP的TG曲线出现3个阶段,并使得后2个失重阶段的初始和终止温度都有所提前。凝聚相分解产物分析表明Ni_0.5Zn_0.5Fe₂O₄加速了凝聚相AP的分解及氨气的释放。含Ni_0.5Zn_0.5Fe₂O₄的AP的高温分解反应的动力学参数E_a=238.88 kJ·mol^-1,A=1018.59 s^-1,动力学方程可表示为dα/dt=10^18.99(1-α)[-ln(1-α)]^3/5e^-2.87×104T。始点温度(T_e)和峰顶温度(T_p)计算得出AP的热爆炸临界温度值分别为:574.83 K和595.41 K。分解反应的活化熵(ΔS^≠)、活化焓(ΔH^≠)和活化能(ΔG^≠)分别为:109.61 J·mol^-1·K^-1、236.49 kJ·mol^-1及172.58 kJ·mol^-1。     

蝎型铜配合物：Cu2[ μ-pz]2[HB(pz)3]2和Cu[B(pz)4]2的合成、结构及热分解动力学性质

本文设计合成了两种以聚吡唑硼酸盐、吡唑为配体的铜配合物Cu₂[ μ-pz]₂[HB(pz)₃]₂(1)和Cu[B(pz)₄]₂(2)(pz：吡唑(C₃H₄N₂))。运用元素分析、红外光谱对配合物进行了表征，并用X-ray衍射测定了它们的晶体结构。非等温热分解动力学研究表明：配合物1的热分解反应分两步，配合物2的热分解反应一步进行。通过计算，配合物1热分解的第一步反应的可能机理为成核与生长，n=1/4；第二步反应的可能机理为化学反应。其非等温动力学方程分别为：dα/dT=A/β e^-E/RT·1/4(1-α)[-ln(1-α)]^-3和dα/dT=A/β e^-E/RT·(1-α)²。分解反应的表观活化能分别是520.37 kJ·mol^-1和149.65 kJ·mol^-1；指前因子lnA分别是118.06 s^-1和28.10 s^-1。配合物2热分解的可能机理为化学反应。其非等温动力学方程为：dα/dT=A/β e^-E/RT·(1-α)²。分解反应的表观活化能是111.41 kJ·mol^-1；指前因子lnA是21.20 s^-1。     

在一维ZnO表面可控构建Co3Mn1纳米晶及其催化CO氧化性能

利用热分解法制备了结构明确的负载型纳米晶催化剂。在纳米晶成核和生长过程中加入一维ZnO纳米棒作为晶种,调控不同组分的纳米晶在 ZnO纳米棒表面均匀生长,从而获得了结构明确的 MnO/ZnO、Co₃O₄/ZnO、Co₃Mn₁/ZnO催化剂。透射电子显微镜(TEM)与 X 射线粉末衍射(XRD)结果显示,不同组分纳米颗粒都均匀分散在 ZnO 纳米棒表面。相对于 MnO/ZnO 和Co₃O₄/ZnO催化剂,Co₃Mn₁/ZnO催化剂在CO氧化反应中具有最佳的催化性能。在200 L·g_cat^-1·h^-1的气时空速下,Co₃Mn₁/ZnO催化剂起活温度为 50 ℃,其 T100(CO 转化率达到 100% 时的温度)为 200 ℃;利用 X 射线光电子能谱(XPS)对不同催化剂进行了分析,结果显示,Co₃Mn₁/ZnO催化剂的氧空位比MnO/ZnO催化剂提高了30%以上,从而使其具有较高的CO氧化催化性能。更为重要的是,Co₃Mn₁/ZnO复合纳米晶催化剂的活化能(39.4 kJ·mol^-1)远低于其它负载型纳米晶催化剂。     

La1-xCaxFeO3-δ系阴极材料的GNP法合成及电性能研究

采用甘氨酸-硝酸盐(GNP)法合成了LaFeO₃及La_1-xCa_xFeO_3-δ(x=0.1～0.5)系列粉体，用TG-DTA、XRD、TEM、SEM等对产物形成过程及微结构进行了表征。结果表明，所合成的系列样品均形成钙钛矿结构的单相固溶体。在x≤20mol%的Ca含量范围内，产物为正交钙钛矿结构；当x>30mol%时，转变为立方钙钛矿相。相同条件下产物的衍射峰强度、晶胞体积及晶粒尺寸都随Ca含量的增大而减小。采用直流四端子法测量了烧结体在中温(450～800 ℃)区的电导率。掺杂使样品导电能力显著增强，电导率随Ca²⁺掺入量的增大先增大后减小，La_0.6Ca_0.4FeO_3-δ样品的电导率最高。在低温段，各样品的导电行为符合小极化子导电机制，导电活化能为13.67～22.70 kJ·mol^-1。     

La2-xBixCuO4阴极材料的合成与电化学性质

采用甘氨酸-硝酸盐法合成了固体氧化物燃料电池阴极材料La_2-xBi_xCuO₄（x=0、0.05、0.10）,并利用X射线衍射（XRD）对材料的物相进行分析。结果表明,La_2-xBi_xCuO₄形成单一的类钙钛矿结构氧化物,且晶胞体积随着铋掺杂量的增加而增大。在950℃烧结24 h过程中,La_2-xBi_xCuO₄不与电解质Sm_0.2Ce_0.8O_1.9（SDC）发生反应,表明这种电解质材料具有良好的高温化学相容性。电导率测试结果表明Bi的掺入显著提高了材料电导率。程序升温脱附测试结果表明,铋的掺杂显著增强了材料的表面氧吸附能力。不同氧分压下的交流阻抗谱测试结果表明,La_1.9Bi_0.1CuO₄阴极在700℃空气中的极化电阻为0.26 Ω·cm²,以电解质SDC支撑的单电池NiO-SDC/SDC/La_1.90Bi_0.10O₄在700℃的最大输出功率密度为308 mW·cm^-2,电极反应的速控步骤为氧分子的扩散与表面吸附过程。     

质子导体BaCe0.4Zr0.4M0.2O3-δ (M=In，Y，Gd，Sm)化学稳定性及电性能

采用高温固相法制备了不同阳离子掺杂的BaCe_0.4Zr_0.4M_0.2O_3-δ (M=In,Y,Gd,Sm)系列质子导体。运用X射线衍射仪、扫描电子显微镜分别对四类质子导体的物相结构、微观形貌进行了表征,应用IM6e型电化学工作站测定了其不同温度下的阻抗谱,并对样品在CO₂和沸水中的稳定性进行了研究。结果表明：除Sm³⁺掺杂的质子导体有少量的杂质相Sm₂O₃外,其他3种均为单相立方晶钙钛矿结构;对CO₂和沸水皆表现良好的化学稳定性;Y³⁺掺杂的质子导体具有高的电导率,800 ℃约为2.07×10^-2 S·cm^-1,空气气氛电导活化能为72.34 kJ·mol^-1。     

复盐K2Zn(IO3)4·2H2O的热化学研究

The standard enthalpy of formation (Δ_fH^?_m［K₂Zn(IO₃)₄·2H₂O,s,298.2K］=-2210.68 kJ·mol^-1) of a double salt K₂Zn(IO₃)₄·2H相似文献   

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.     

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.     

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.     

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。     

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.     

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.     

Preparation and structure of NaSr0.5Al2B2O7 and NaCa0.5Al2B2O7

Two compounds NaSr_0.5Al₂B₂O₇ and NaCa_0.5Al₂B₂O₇, have been found to crystallize into a new structure type by Rietveld refinement from X-ray powder diffraction data. Their structure belongs to hexagonal space group P6₃/m, with lattice parameters of , for NaSr_0.5Al₂B₂O₇ and , for NaCa_0.5Al₂B₂O₇, respectively. The structure is built up by [Al₂B₂O₇]²⁻ double layer and Na⁺/Ca²⁺ or Na⁺/Sr²⁺ ions alternatively stacking along the c-axis. The sites in the inter-double layer are fully occupied jointly by Na and Ca or Sr, but the intra-double layer sites are only half occupied solely by Na. A mechanism of the transition of the structure from CaAl₂B₂O₇ to present structure type by replacing only 1% Ca by Na (2%) as observed by Chang and Keszler (Mater. Res. Bull. 33 (1998) 299) is also proposed.     

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.