La0.7Sr0.3Co1-xFexO3催化剂氮氧化物储存及抗硫性能

采用溶胶-凝胶法通过在静态空气中700°C焙烧制备了不同Fe掺杂量的La0.7Sr0.3Co1-xFexO3(x=0,0.2,0.6,1.0)系列钙钛矿催化剂.考察了Fe掺杂量对催化剂的结构、氮氧化物储存、抗硫及再生性能的影响.研究结果表明:在La0.7Sr0.3CoO3钙钛矿B位用Fe部分取代Co,可有效提高SrCO3物相的分散,X射线衍射(XRD)结果显示样品中基本为钙钛矿物相.随着Fe掺杂量的增加,催化剂的NOx储存量(NSC)下降.对预硫化样品进行NOx储存测试,发现La0.7Sr0.3CoO3催化剂由于表面沉积了硫酸盐,同时钙钛矿结构也遭到了部分破坏,使得NOx储存量和NO氧化能力均大幅度下降,NOx储存量下降了64.2%,NO-to-NO2转化率从72.8%降至43.4%.掺杂Fe元素后,催化剂的抗硫性能都有不同程度的提高,特别是Fe掺杂量为60%的样品具有最佳的抗硫性能和可再生性能.与新鲜样品相比较,再生后样品的NOx储存量仅下降16.6%,而NO-to-NO2转化率为69.1%,几乎与新鲜样品相同.     

固体氧化物燃料电池La0.7Sr0.3Cr1-xMnxO3-δ阳极性能研究

采用溶胶凝胶法制备了La0.7Sr0.3Cr1-xMnxO3-δ(x=0.3,0.4,0.5,0.6)系列阳极粉体。在1000℃下焙烧后,XRD结果显示粉体物相为单一的钙钛矿相。制备以La0.7Sr0.3Cr1-xMnxO3-δ为阳极,Ce0.8Sm0.2O1.9(SDC)为电解质,Pr0.6Sr0.4Co0.8Fe0.2O3-δ-SDC复合阴极的电解质支撑型固体氧化物燃料单电池。由扫描电子显微镜(SEM)观察表明单电池电解质致密,阳极孔径分布均匀,厚度约为20μm,多孔阴极厚度为10μm。采用直流四电极法测试以La0.7Sr0.3Cr0.5Mn0.5O3-δ为阳极用湿氢气作燃料时在800℃下获得最大输出功率为232.84 mW.cm-2,短路电流为0.92 A.cm-2。     

低温熔盐法制备球状多孔 La1-xSrxMn0.8Fe0.2O3（0≤x≤0.6）及其催化 CO氧化性能

汽车尾气中 CO, HC, NOx,硫化物及其颗粒粉尘严重危害人们身体健康和大气环境,是大气环境的主要污染源之一.目前,尾气净化是其减排的最主要方式.汽车尾气催化剂的发展经历了几代的研究,一直以来广泛采用 Pt, Pd和 Rh等贵金属,但因其资源匮乏,价格昂贵,容易被 S和 P中毒,因此人们逐渐将目光投向非贵金属催化剂的研发.钙钛矿复合氧化物因具有独特的物理化学性质以及灵活的“化学剪裁”特性而在材料研究等领域颇受青睐,有望成为贵金属催化剂的替代品.一般而言,催化剂的比表面积越大,表面活性位点越多,其催化活性越高,且会明显降低起燃温度.目前,一些制备工艺,如水热法、共沉淀法、微乳液法和硬模板法,虽可在一定程度上提高催化剂的比表面积,但却存在费时、耗能及制备工艺复杂等缺点.因此,如何简单有效地制备出大比表面积的钙钛矿型催化剂依然是一个难题.本文以合成的分级多孔δ-MnO2微球为模板,采用熔盐法制备出球状多孔 La1-xSrxMn0.8Fe0.2O3(0≤x≤0.6)钙钛矿氧化物,研究了球状多孔钙钛矿氧化物的形成过程和合适的制备温度,以及 B位 Fe3+掺杂量为20%时 A位 Sr2+掺杂量对钙钛矿催化剂结构和催化活性的影响.采用 X射线粉末衍射、扫描电子显微镜、透射电子显微镜、N2吸附-脱附、傅里叶红外光谱(FT-IR)和 X射线能谱(XPS)等方法对催化剂进行了表征.在固定床石英管反应器上评价了催化剂催化 CO氧化活性及稳定性,采用气相色谱联接氢火焰离子化检测器检测了产物和反应物的组成.结果表明,以分级多孔δ-MnO2微球为模板,采用熔盐法在450oC反应4 h制备出的球状多孔 La1-xSrxMn0.8Fe0.2O3(0≤x≤0.6)钙钛矿氧化物具有良好的结晶性、较大的比表面积(55.73 m2/g)和孔体积(0.37 cm3/g).其球状多孔结构的形成可分为两个阶段：原位形成钙钛矿相和纳片表面析出钙钛矿晶粒及钙钛矿晶粒的再生长.另外, FT-IR光谱表明, Fe3+和 Sr2+成功进入 A, B位.同时, CO转化曲线表明, B位 Fe3+的掺杂量为20%时, A位 Sr2+的掺杂量高于30%时可以明显改善催化剂催化 CO氧化活性： La1-xSrxMn0.8Fe0.2O3(0≤x≤0.3)的T50和T90分别在180和198oC左右;而 La0.55Sr0.45Mn0.8Fe0.2O3和 La0.4Sr0.6Mn0.8Fe0.2O3的T50均低于125oC; La0.55Sr0.45Mn0.8Fe0.2O3的T90为181oC,而 La0.4Sr0.6Mn0.8Fe0.2O3却仍低于125oC. XPS结果则证明,较高的催化活性得益于 La0.4Sr0.6Mn0.8Fe0.2O3表面存在较多的 Mn4+、氧空位及吸附氧.最后, La0.55Sr0.45Mn0.8Fe0.2O3和 La0.4Sr0.6Mn0.8Fe0.2O3的稳定性测试结果表明,采用熔盐法以δ-MnO2为模板在450oC焙烧4 h制备的多孔球状钙钛矿具有较好的催化稳定性.虽然催化剂制备工艺简单,周期短,但比表面积最大只有55.73 m2/g,为硬模板法的1/2,因此提高比表面积将是今后研究的方向.     

纳米La0.8A’0.2Mn1-xCuxO3（A’=Ce and/or Sr）的制备、表征及其高效催化NO+CO的性能研究

采用柠檬酸-溶胶凝胶法制得钙钛矿型复合氧化物La0.8Ce0.2Mn1-xCuxO3(x=0.2,0.3,0.4),La0.8Sr0.2Mn0.6Cu0.4O3,La0.8Ce0.1Sr0.1Mn0.6 Cu0.4 O3,并采用X射线衍射(XRD)、扫描电镜(SEM)、比表面积(BET)、X射线光电子能谱(XPS)对其进行表征,测试了复合氧化物对CO+NO的催化活性。结果表明:La0.8Ce0.1Sr0.1Mn0.6Cu0.4O3催化活性最好,150℃时CO转化率91.8%,300℃时NO转化率100%;对于La0.8Ce0.2Mn1-xCuxO3(x=0.2,0.3,0.4),比表面积和颗粒的大小及分散度是影响催化活性的主要因素;对于La0.8Ce0.2Mn0.6Cu0.4O3,La0.8 Sr0.2 Mn0.6 Cu0.4 O3,La0.8 Ce0.1 Sr0.1 Mn0.6 Cu0.4 O3,催化剂的组成是影响催化活性的关键因素。     

焙烧温度对LaSrFeMo_(0.9)Co_(0.1)O_6催化甲烷燃烧性能的影响

采用溶胶凝胶法制备La Sr Fe Mo0.9Co0.1O6,以催化甲烷燃烧为目标反应,研究不同焙烧温度(600、700、800、900℃)对其催化甲烷燃烧性能的影响。通过XRD、BET、H2-TPR及SEM技术对其结构进行表征。结果表明,在不同的焙烧温度下均可形成完整的双钙钛矿晶型,且焙烧温度不同其催化活性不同,随着焙烧温度的升高其催化活性先升高后逐渐降低。当焙烧温度为800℃,样品比表面积为14 m2/g,起燃温度Tl0%为428℃,T90%为640℃。     

La0.75Sr0.25Cr0.5Mn0.5O3的制备及其NO2气敏性能

利用高温固相反应法和溶胶-凝胶法制备了La0.75Sr0.25Cr0.5Mn0.5O3钙钛矿复合氧化物粉体。采用XRD,TEM对粉体物相组成及颗粒形貌进行表征,并以制备的两种粉体作为敏感材料分别制成管状传感器,测试了其NO2气敏性能。结果表明：采用高温固相反应法和溶胶-凝胶法在不同焙烧温度下,均可制得单相La0.75Sr0.25Cr0.5Mn0.5O3粉体,采用溶胶-凝胶法在800℃焙烧2 h得到的粉体粒径约为20 nm;传感器输出电动势信号对NO2浓度之间呈良好的线性关系;溶胶-凝胶法制得粉体的气敏性能优于高温固相反应法制得粉体的气敏性能。     

不同金属取代六铝酸盐的制备及其对甲烷燃烧的催化性能研究

采用铝溶胶作为碳酸铵共沉淀的前驱体,结合乙醇超临界干燥制备了不同金属取代六铝酸盐催化剂(Ba0.8La0.2MAl11O19-α,M=Mn,Fe,Co,Cu),并用BET,XRD,TEM,UV-Vis和O2-TPD等技术对催化剂进行了表征。结果表明,经1200℃焙烧后,生成了具有大的比表面积(42~73 m2.g-1)的棒状六铝酸盐,比表面积由大到小的顺序是Mn>Co>Fe>Cu。XRD结果表明,除Mn取代催化剂之外,其他均含有少量-αAl2O3杂质相。Fe,Mn取代六铝酸盐中的金属离子(Fe3+,Mn3+)主要为Oh配位,而Co,Cu取代六铝酸盐中的金属离子(Co3+,Cu2+)则为Oh和Td配位。O2-TPD表明,Mn,Cu取代的催化剂中具有高的晶格氧含量。催化剂活性由高到低的顺序为Mn>Cu>Fe>Co,催化活性取决于过渡金属离子的氧化还原循环的可逆性、比表面积以及晶格氧等因素。     

La_xSr_(1-x)FeO_3催化剂的制备及其催化还原SO_2性能的研究

采用柠檬酸配合溶胶凝胶法制备了不同La、Sr比例的La_xSr_(1-x)FeO_3催化剂样品,通过X射线衍射(XRD)、比表面积测定(BET)、CO-程序升温还原(CO-TPR)、SO2-程序升温脱附(SO2-TPD)、O2-程序升温脱附(O2-TPD)的方法对催化剂的结构和物理化学性质进行了表征.综合表征结果分析,通过柠檬酸配合法成功制得了具有典型钙钛矿结构的LaxSr1-xFe O3系列复合氧化物;在La Fe O3的结构中A位(La)掺杂替换少量的Sr,可以增大催化剂的比表面积、提高氧化物结构中氧空位的数量、促进反应气体在催化剂中完成反应,大大提升了SO2的催化还原转化效率.实验结果表明,当x为0.8时,CO催化还原SO2的转化率最高,在空速为24 000 m L/(g·h),温度600℃时,转化率达到95%,取得了良好的催化效果.     

复合阴极材料La1-xSrxCuO3-δ-SDC的制备及电学性能

合成具有单相正交钙钛矿结构的La1-xSrxCuO3-δ(x=0.15, 0.2, 0.3, 0.4)系列样品, 碘量滴定法实验结果表明, 随着Sr掺入量的增加, Cu3+离子的含量逐渐增加. 电学性能研究结果表明, La0.7Sr0.3CuO3-δ电导率最高, 与La0.6Sr0.4CoO3-δ相比, La0.7Sr0.3CuO3-δ具有更好的电化学性能, 可作为一种新的中温固体氧化物燃料电池(IT-SOFC)阴极材料. 将La0.7Sr0.3CuO3-δ与不同质量比的中温电解质Ce0.85Sm0.15O2-δ(SDC) 固相混合, 制备复合阴极材料, 电化学性能测试结果表明, 掺入适量的SDC有利于降低La0.7Sr0.3CuO3-δ电极的极化, 获得性能更优越的IT-SOFC阴极材料, 提高在中温区单电池的输出功率.     

还原剂对La0.7Sr0.3Co0.8Fe0.2O3钙钛矿催化剂NOx储存性能的影响

采用溶胶-凝胶法制备了La0.7Sr0.3Co0.8Fe0.2O3钙钛矿催化剂,考察了还原剂种类(CO,C3H6,H2)对催化剂在氮氧化物储存还原(NSR)循环前后的氮氧化物储存量(NSC)和NO-to-NO2转化率的影响.O2程序升温脱附(O2-TPD)实验结果表明,CO还原后的钙钛矿催化剂上形成了较多的氧空位,而氧空位则是一种有效的NOx储存活性中心.活性测试和傅里叶红外变换(FTIR)光谱表征结果显示:在NSR循环中,以CO为还原剂时催化剂显示了最佳的氮氧化物(NOx)储存效果.进一步的研究结果显示,当采用CO作为还原剂时,经过三次NSR循环后,催化剂中出现了Sr3Fe2O7新物相,而该物相可能具有比La0.7Sr0.3Co0.8Fe0.2O3钙钛矿更佳的NOx储存性能.综上所述,CO作为还原剂时可能使钙钛矿催化剂产生更多的氧空位以及更易于储存NOx的Sr3Fe2O7物相,这些原因使其NOx储存性能得到了大幅度改善.     

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.     

Li1.2Mn0.54Ni0.13Co0.13O2正极材料的Ga2O3包覆改性及电化学性能

首先采用共沉淀方法制备富锂锰基正极材料 Li_1.2Mn_0.54Ni_0.13Co_0.13O₂原始样品(P-LRMO), 然后通过简单的湿化学法以及低温煅烧方法对其进行不同含量 Ga₂O₃原位包覆。透射电子显微镜(TEM)以及 X射线光电子能谱(XPS)结果表明在 P-LRMO表面成功合成了 Ga₂O₃包覆层。电化学测试结果表明:含有 3 %Ga₂O₃的改性材料 G3-LRMO具有最优的电化学性能, 其在 0.1C倍率(电流密度为 25 mA·g^-1)下首圈充放电比容量可以达到 270.1 mAh·g^-1, 在 5C倍率下容量仍能保持 127.4 mAh·g^-1, 优于未改性材料的 90.7 mAh·g^-1, 表现出优异的倍率性能。G3-LRMO在 1C倍率下循环 200圈后仍有 190.7 mAh·g^-1的容量, 容量保持率由未改性前的 72.9 %提升至 85.6 %, 证明 Ga₂O₃包覆改性能有效提升富锂锰基材料的循环稳定性。并且, G3-LRMO在 1C倍率下循环 100圈后, 电荷转移阻抗(R_ct)为 107.7 Ω, 远低于未改性材料的 251.5 Ω, 表明 Ga₂O₃包覆层能提高材料的电子传输速率。     

Investigation of phase equilibria in the systems K2SO4Sc2(SO4)3, Rb2SO4Sc2(SO4)3 and Cs2SO4Sc2(SO4)3

Phase diagrams of the systems K₂SO₄Sc₂(SO₄)₃, Rb₂SO ₄Sc₂(SO₄)₃ and Cs₂SO₄ Sc₂(SO₄)₃ have been investigated by X-ray diffraction phase analysis and differential thermal analysis techniques. A salient feature of all the systems is the formation of M₃Sc(SO₄)₃, which melt incongruently, and MSc(SO₄)₂, which on heating decompose in the solid state.     

Synthesis and molecular structures of heptafluoroisopropylated fullerenes: C60(i-C3F7)8, C60(i-C3F7)6, and C60(CF3)2(i-C3F7)2

One isomer of C₆₀(i-C₃F₇)₈, three isomers of C₆₀(i-C₃F₇)₆, and the first mixed perfluoroalkylated fullerene, C₆₀(CF₃)₂(i-C₃F₇)₂, have been isolated by HPLC from a mixture prepared by reaction of C₆₀ with heptafluoroisopropyl iodide in a glass ampoule at 260-290 °C. The molecular structures of the four new compounds have been determined by means of X-ray single crystal diffraction partially also by use of synchrotron radiation. Theoretical calculations at the DFT level of theory have been employed to rationalize the energetics of isomers and of C₆₀-R_f binding.     

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.     

Syntheses, structures, and properties of Ag4(Mo2O5)(SeO4)2(SeO3) and Ag2(MoO3)3SeO3

Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) has been synthesized by reacting AgNO₃, MoO₃, and selenic acid under mild hydrothermal conditions. The structure of this compound consists of cis-MoO₂²⁺ molybdenyl units that are bridged to neighboring molybdenyl moieties by selenate anions and by a bridging oxo anion. These dimeric units are joined by selenite anions to yield zigzag one-dimensional chains that extended down the c-axis. Individual chains are polar with the C₂ distortion of the Mo(VI) octahedra aligning on one side of each chain. However, the overall structure is centrosymmetric because neighboring chains have opposite alignment of the C₂ distortion. Upon heating Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) looses SeO₂ in two distinct steps to yield Ag₂MoO₄. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): orthorhombic, space group Pbcm, a=5.6557(3), b=15.8904(7), c=15.7938(7) Å, V=1419.41(12), Z=4, R(F)=2.72% for 121 parameters with 1829 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ was synthesized by reacting AgNO₃ with MoO₃, SeO₂, and HF under hydrothermal conditions. The structure of Ag₂(MoO₃)₃SeO₃ consists of three crystallographically unique Mo(VI) centers that are in 2+2+2 coordination environments with two long, two intermediate, and two short bonds. These MoO₆ units are connected to form a molybdenyl ribbon that extends along the c-axis. These ribbons are further connected together through tridentate selenite anions to form two-dimensional layers in the [bc] plane. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): monoclinic, space group P2₁/n, a=7.7034(5), b=11.1485(8), c=12.7500(9) Å, β=105.018(1) V=1002.7(2), Z=4, R(F)=3.45% for 164 parameters with 2454 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ decomposes to Ag₂Mo₃O₁₀ on heating above 550 °C.     

Luminescence properties of efficient X-ray phosphors of YBa3B9O18, LuBa3(BO3)3, α-YBa3(BO3)3 and LuBO3

The samples of YBa₃B₉O₁₈, LuBa₃(BO₃)₃, α-YBa₃(BO₃)₃ and LuBO₃ powders have been synthesized by the solid-state reaction methods at high temperature and their X-ray excited luminescent properties were investigated. All the studied materials show a broad emission band in the wavelength range of 300-550 nm with the peak centers at about 385 nm for YBa₃B₉O₁₈ and LuBa₃(BO₃)₃, 415 nm for α-YBa₃(BO₃)₃ and 360 nm for LuBO₃ powders, respectively. Even though those compounds have the different atomic structures, they have the common structural feature of each yttrium or lutetium ion bonded to six separate BO₃ groups, i.e., octahedral RE(BO₃)₆ (RE=Lu or Y) moiety. This octahedral RE(BO₃)₆(RE=Lu or Y) moiety seems to be an important structural element for efficient X-ray excited luminescence of those compounds, as are the edge-sharing octahedral TaO₆ chains for tantalate emission.     

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.     

A new three-dimensional cobalt phosphate: Co5(OH2)4(HPO4)2(PO4)2

A three-dimensional (3D) cobalt phosphate: Co₅(OH₂)₄(HPO₄)₂(PO₄)₂ (1), has been synthesized by hydrothermal reaction and characterized by single-crystal X-ray diffraction, thermogravimetric analysis, and magnetic techniques. The title compound is a template free cobalt phosphate. Compound 1 exhibits a complex net architecture based on edge- and corner-sharing of CoO₆ and PO₄ polyhedra. The magnetic susceptibility measurements indicated that the title compound obeys Curie-Weiss behavior down to a temperature of 17 K at which an antiferromagnetic phase transition occurs.     

Synthesis and crystal structure of gallosilicate- and aluminogermanate tetrahydroborate sodalites Na8[GaSiO4]6(BH4)2 and Na8[AlGeO4]6(BH4)2

Tetrahydroborate enclathrated sodalites with gallosilicate and aluminogermanate host framework were synthesized under mild hydrothermal conditions and characterized by X-ray powder diffraction and IR spectroscopy. Crystal structures were refined in the space group P-43n from X-ray powder data using the Rietveld method. Na₈[GaSiO₄]₆(BH₄)₂: a=895.90(1) pm, V=0.71909(3)×10⁻⁶ nm³, R_P=0.074, R_B=0.022, Na₈[AlGeO₄]₆(BH₄)₂: a=905.89(2) pm, V=0.74340(6)×10⁻⁶ nm³, R_P=0.082, R_B=0.026. The tetrahedral framework T-atoms are completely ordered in each case and the boron atoms are located at the centre of the sodalite cages. The hydrogen atoms of the enclathrated anions were refined on x, x, x positions, restraining them to boron-hydrogen distances of 116.8 pm as found in NaBD₄.The IR-absorption spectra of the novel phases show the typical bands of the tetrahedral group as found in the spectrum of pure sodium boron hydride.The new sodalites are discussed as interesting -containing model compounds which could release pure hydrogen.