PW11M(M=Cu、Co)@TiO2多相催化剂的制备及氧化脱硫性能

摘要：以过渡金属(Cu, Co)取代磷钨酸为模板剂，硫酸钛为钛源，通过一步模板法合成出一类多酸基PW11M(M=Cu、Co)@TiO2材料，采用FT-IR、XRD、XPS、Raman、SEM和TEM表征手段对材料进行了结构表征. 结果表明，PW11M(M=Cu、Co)被引入到TiO2中，形成了球形核壳结构. N2吸附-脱附测试表明，PW11Co@TiO2具有介孔结构:孔径大小为3.3 nm，比表面积为72.4 m2/g. 在以H2O2为氧化剂，乙腈为溶剂的氧化脱硫反应体系中考察了其催化活性，结果表明：复合材料PW11M(M=Cu、Co)@TiO2表现出良好的催化性能. 其中催化剂PW11Co@TiO2在投入量为40 mg，反应底物为500 ppm，反应温度60 oC，反应40 min后，DBT的脱硫率达到99.7%. 中断和循环实验表明，催化剂PW11Co@TiO2具有良好的稳定性，在相同的反应条件下，循环反应5次后，催化剂的催化活性没有明显下降.     

模板法制备催化剂PW12@Fe-TiO2及其催化氧化脱硫性能

采用模板法一步合成了一类多酸基PW_(12)@Fe-TiO_2材料,利用Raman、XRD、XPS和SEM表征手段对材料进行了结构表征。结果表明,磷钨酸(PW_(12))被包埋到Fe-TiO_2中,形成球形结构。N_2吸附-脱附测试显示,PW_(12)@Fe-TiO_2为介孔材料:孔径尺寸为4.1 nm,比表面积为30.3 m~2·g~(-1)。所合成材料作为催化剂,以H_2O_2为氧化剂,乙腈为溶剂,在模拟油的氧化脱硫反应体系中表现出较好的催化性能。当PW_(12)@Fe-TiO_2的加入量为40 mg,反应底物为5.0 mL,反应温度60 ~oC,反应到40 min时,DBT的去除率到达了99.9%。中断和循环实验结果表明,催化剂PW_(12)@Fe-TiO_2具有良好的稳定性,在相似的反应条件下,循环使用5次,催化剂的催化活性依然保持不变。     

过渡金属对选择性催化还原脱硝CeO_2@TiO_2催化剂低温活性的促进作用

采用过渡金属M(M=Mn、Co、Fe和Cu)掺杂改性自发沉积策略制备的非晶态CeO_2@TiO_2催化剂,考察M-CeO_2@TiO_2选择性催化还原NO_x的低温活性,并通过XRD、TEM、N2吸附-脱附、H2-TPR、NH3-TPD及in-situ FT-IR等表征手段研究M-CeO_2@TiO_2的结构、表面性质以及低温NH3-SCR反应过程。结果表明,M-CeO_2@TiO_2具有更优异的低温氧化还原能力以及更多的表面酸量,且Cu掺杂对CeO_2@TiO_2选择性催化还原NO_x低温活性具有最为显著的促进作用。Cu-CeO_2@TiO_2催化剂在低温NH3-SCR反应过程中同时存在E-R机理和L-H机理,但是由于"快速SCR"使得L-H机理反应起关键作用。     

氨基化磁性Fe3O4@Cu3(BTC)2材料的合成及其在Knoevenagel缩合中的催化性能

金属有机骨架材料具有大比表面积、高孔隙率、热稳定性好、规整且可调控的孔结构、易于功能化的骨架金属离子和有机配体等优点,是制备多相催化剂的重要材料之一.虽然减小金属有机骨架材料等多孔材料的粒径可以提高反应物的传质效率,从而提高其催化活性;但是,纳米尺寸催化剂的分离和回收困难.将磁性纳米粒子和金属有机骨架材料结合制备具有核-壳结构的磁性金属有机骨架材料是解决上述问题的有效方法.此类材料兼具磁性材料和金属有机骨架材料的双重优势,既可以磁性分离,又具有金属有机骨架材料的催化活性.而且,厚度可控的壳层材料表现出与纳米催化剂相当甚至更好的催化活性.我们采用逐层自组装方法制备了核-壳结构的磁性Fe3O4@Cu3(BTC)2复合材料,并对材料进行氨基化修饰,制备了基于金属有机骨架材料的磁性多相碱催化剂.采用粉末X射线衍射(XRD)、傅里叶变换红外光谱(FT-IR)、透射电镜(TEM)、扫描电镜(SEM)、氮气吸附等方法对材料的组成和结构进行了表征,并考察了材料在Knoevenagel缩合反应中的催化性能.首先采用粉末XRD表征材料的晶体结构.在复合材料Fe3O4@Cu3(BTC)2的XRD谱中,同时出现了Fe3O4和Cu3(BTC)2的特征衍射峰.采用氨基配体修饰后,材料的XRD谱没有明显变化,说明修饰后的材料保持了Fe3O4@Cu3(BTC)2的晶体结构.透射电镜结果表明,包裹25次得到的磁性复合材料Fe3O4@Cu3(BTC)2是以Fe3O4为核心,以Cu3(BTC)2为壳的核-壳结构,壳层厚度大约为200 nm.氨基修饰后,材料的透射电镜图相对修饰前无明显变化.扫描电镜结果表明,合成的Fe3O4为球形结构,粒径为100-600 nm.采用Cu3(BTC)2进行包裹后,在Fe3O4表面生长了由Cu3(BTC)2纳米颗粒组成的壳层.采用氨基配体修饰后,材料的形貌无明显改变.进一步采用氮气吸附表征材料的孔结构并测定材料的比表面积和孔体积.结果表明,由于大比表面的Cu3(BTC)2的引入,复合材料Fe3O4@Cu3(BTC)2的比表面积增大为462 m2/g,孔体积为0.38 cm3/g.氨基修饰后,材料的比表面积和孔体积都有较大程度的降低,说明配体分子占据了壳层材料Cu3(BTC)2中的纳米孔道.采用苯甲醛和氰基乙酸乙酯的Knoevenagel缩合反应作为模型,考察了材料的催化活性.研究发现,Fe3O4对此反应几乎没有活性,Fe3O4@Cu3(BTC)2给出了中等的催化活性.在材料上引入氨基后,由于氨基和Cu3(BTC)2上的Lewis酸性位点的协同效应,在很大程度了提高了材料的催化活性.溶剂效应实验结果表明,反应溶剂对材料的活性和选择性具有较大影响,极性或质子性溶剂有利于反应的进行.多相催化剂的循环稳定性是其重要评价指标之一.热过滤实验结果表明,滤液中无催化活性,反应中的催化活性来源于固体材料,此催化反应为多相催化.随后考察了材料的循环稳定性.虽然氨基化Fe3O4@Cu3(BTC)2材料在溶剂DMSO中表现出最高的催化活性,但XRD和电镜表征结果表明,材料在DMSO中结构遭到破坏,因此循环过程中催化剂的活性损失严重.然后考察了氨基化材料在乙醇中的循环稳定性,发现材料在乙醇中表现出较好的循环稳定性.通过简单磁性分离进行催化剂的分离和回收,催化剂循环使用3次而没有明显的活力损失.而且,XRD和电镜表征结果显示,催化剂的结构在反应过程中没有遭到明显破坏.     

单过渡金属配位磷钨酸铵盐的合成及其催化环己酮氨肟化

以磷钨酸和过渡金属盐在pH值为4.0~5.0的条件下合成了4种具有Keggin结构的单过渡金属配位磷钨酸铵盐NH4MPW11(M=Zr2+,Co2+,Ni2+,Cu2+),通过红外、紫外、热重、X射线衍射、循环伏安法等技术对这类杂多化合物的结构和性质进行了表征,并考察了它们在环己酮氨肟化反应中的催化性能.结果表明:单过渡金属配位的磷钨酸铵盐NH4MPW11(M=Zr2+,Co2+,Ni2+,Cu2+)具有典型的Keggin结构,过渡金属离子配位后,热稳定性和氧化性增强;在催化环己酮氨肟化反应中,NH4MPW11的催化性能低于单缺位磷钨酸铵盐(NH4PW11),其中NH4ZrPW1 1为催化剂,性能优于M=Co2+,Ni2+,Cu2+的催化剂,环己酮的转化率达到85.1%,环己酮肟的选择性达到92.1%,而NH4CuPW11的催化性能则下降显著;H2O2的分解实验表明,过渡金属配位的磷钨酸铵盐对H2O2分解均存在一定的促进作用,分解能力随过渡金属种类而变化,其中NH4CuPW1 1对H2O2的分解率高达72.3%,这是造成过渡金属配位的磷钨酸铵盐在环己酮氨肟化反应中催化性能下降的主要原因;回收催化剂的红外和XRD表征表明,氨肟化反应后的NH4MPW11保持了Keggin型的一级结构,但二级结构遭到一定程度的破坏.     

磁铅石型复合氧化物LaNi_xCo_(1-x)Al_(11)O_(19+δ)催化剂上CH_4和CO_2重整反应的研究

考察了磁铅石型复合氧化物LaNi_(0.5)M_(0.5)Al_(11)O_(19 + δ) (M = Co, Fe, Mn, Cu)和LaNi_xCo_(1-x)Al_(11)O_(19+δ)催化剂在CH_4与CO_2重整制合成 气反应中的催化活性，并应用XRD，TPR，UV-DRS技术着重表征LaNi_xCo_(1-x)Al_ (11)O_(19+δ)催化剂的结构和性能。研究结果表明该系列催化剂具有相同的晶体 结构和相似的还原稳定性。对不同过渡金属取代的催化剂来说，以LaNi_(0.5)Co_ (0.5)Al_(11)O_(19+δ)催化剂具有最好的反应活性。而对于LaNi_xCo_(1-x)Al_ (11)O_(19+δ)系列催化剂，当x ≤ 0.375时，随x值的增大，催化活性明显提高， 但在0.375 ≤ x ≤ 1.0范围内，催化活性几乎保持不变。由此得到结论，对于此 反应来说，控制Ni量在0.375 ≤ x ≤ 0.50范围内比较合适。     

第四周期过渡金属钨磷杂多酸盐的合成及表征(C)

合成了Keggin型缺位取代杂多酸盐(Na5PW11Z(H2O)O39,Z=Mn、Fe、Co、Ni、Cu、Zn,以下简称PW11Z)催化剂.通过ICP、IR、UV等表征手段对催化剂进行了表征.元素分析结果表明,各缺位取代杂多酸盐的计量式为Na5PW11Z(H2O)O39.IR光谱表明,取代型杂多化合物仍保持Keggin型骨架结构.而且,除了Na5PW11Ni(H2O)O39以外,其余化合物的P-O键吸收峰发生劈裂,其劈裂强度为PW11Cu>PW11Zn>PW11Mn>PW11Fe>PW11Co.Mo=O键的振动向低波数位移.UV表征结果表明,由于过渡金属的引入,相对于Keggin型杂多酸H3PW12O40,取代产物的紫外可见吸收峰向紫外方向位移,但位移强度不大,基本有与H3PW12O40中Mo=O键的ππ*跃迁大致相同的吸收.还利用以上催化剂对正己醇氧化生成正己醛的反应活性进行了考察.     

采用金属有机骨架材料M(HBTC)(4,4'-bipy)·3DMF(M=Ni,Co,Zn)催化CO2与环氧丙烷的环加成反应

采用溶剂热法合成了三种M(HBTC)(4,4’-bipy)·3DMF (M = Ni, Co, Zn, HBTC = 1,3,5-均苯三甲酸, 4,4’-bipy = 4,4′-联吡啶)结构的支柱层金属有机骨架材料(MOFs). 首次采用溶剂热和微波法合成了Zn(HBTC)(4,4’-bipy)·3DMF, 并采用多种物理化学方法对其进行了表征. M(HBTC)(4,4’-bipy)·3DMF中包含有M2+离子的蜂窝网格层和BTC单元, BTC单元与4,4’-联吡啶柱进一步交联形成三维多孔骨架材料. 在采用烷基铵卤化物作为助催化剂和无溶剂的条件下, 所有MOFs材料均对催化固定CO2与环氧化合物环加成制备环状碳酸酯反应表现出非常好的协同催化性能, 其催化活性高低顺序为: Zn ＞ Co ＞Ni, 这可通过酸-碱双功能特性进行解释. 采用微波法合成的Zn(HBTC)(4,4’-bipy)·3DMF材料表现出与常规催化剂相似的物理化学性质和催化性能. 考察了不同制备参数的影响和材料的重复使用性能, 并提出了该反应的可能机理.     

Cu_xCo_(1-x)/Al_2O_3/FeCrAl整体式催化剂上甲苯催化燃烧(英文)

以FeCrAl合金薄片为基底,Al2O3浆料为过渡胶体,不同摩尔比的Cu、Co为催化活性组分,制备了一系列CuxCo1-x/Al2O3/FeCrAl(x=0-1)新型整体式催化剂.采用X射线粉末衍射(XRD),扫描电子显微镜(SEM),X光电子能谱(XPS)和程序升温还原(TPR)等手段对催化剂的结构进行了表征.在微型固定床反应器上评价了催化剂的催化甲苯燃烧性能.研究结果表明:在所制备的整体式催化剂上,当Cu含量比较低时,形成了Cu-Co-O固溶体;当Cu含量比较高时,可以测得CuO的衍射峰.催化剂表面颗粒大小和形貌与Cu、Co摩尔比密切相关.在催化剂表面,Co以Co2+和Co3+价态存在,而Cu主要以Cu2+价态存在.催化剂中的Cu可以改善Co的氧化还原性,从而有利于催化剂活性的提高.在所制备的催化剂中,Cu0.5Co0.5/Al2O3/FeCrAl催化剂具有最好的活性,甲苯在374oC可以完全催化燃烧消除.     

M/(MgO)y(CeO2)1－y(M=Ni、Co、Cu)催化剂的催化甲烷燃烧性能

采用溶胶凝胶法制备了M/(MgO)_y(CeO2)_1－y(M=Ni、Co、Cu)催化剂. 研究了催化剂Ni/(MgO)y(CeO₂)_1－y催化活性与Ce含量的关系, 当y＝0.9时, 催化剂的活性和稳定性最好. 对比研究了(MgO)_0.9(CeO2)_0.1为载体, 负载Ni、Co、Cu活性组分的催化剂催化甲烷燃烧性能. 结果表明, 负载Cu的催化剂活性最好, 但二次评价后催化剂已烧结；负载Ni的催化剂活性与负载Cu的催化剂相差不大, 且稳定性最好, 经1000 ℃焙烧的Ni/(MgO)_0.9(CeO2)_0.1催化剂比表面仍有14.32 m₂•g^－1, 具有较高的催化活性和很好的热稳定性；负载Co的催化剂活性不如前两者, 稳定性居中, 但比表面降低得最少, 抗烧结能力强.     

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.     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

Raman scattering investigations on lanthanum-doped Bi4Ti3O12-SrBi4Ti4O15 intergrowth ferroelectrics

The ferroelectric ceramics of Bi₄Ti₃O₁₂, SrBi₄Ti₄O₁₅, and lanthanum-doped Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅ were synthesized, and their Raman spectra were investigated. La-doping resulted in the enlargement of remnant polarization of Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The structure of the Bi₂O₂ layers and TiO₆ octahedra of the intergrowth was found to be different from those of Bi₄Ti₃O₁₂ and SrBi₄Ti₄O₁₅. La³⁺ ions exhibit pronounced selectivity for the occupation of A site as La content is lower than 0.50, and tend to be incorporated into Bi₂O₂ layers when the La content is higher than 0.50. Lanthanum substitution brings about the structural phase transition in Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The variation of ferroelectric property may be attributed to combined contribution from the decreasing of the oxygen vacancies, the relaxation of the lattice distortion, the destroying of the insulation and the space charge compensation effects of the Bi₂O₂ slabs.     

A new 2212-type stair like structure: Bi14Sr21Fe12O61, m=5 member of the generic [Bi2Sr3Fe2O9]m[Bi4Sr6Fe2O16] family

A new oxide, Bi₁₄Sr₂₁Fe₁₂O_61, with a layered structure derived from the 2212 modulated type structure Bi₂Sr₃Fe₂O₉, was isolated. It crystallizes in the I2 space group, with the following parameters: a=16.58(3) Å, b=5.496(1) Å, c=35.27(2) Å and β=90.62°. The single crystal X-ray structure determination, coupled with electron microscopy, shows that this ferrite is the m=5 member of the [Bi₂Sr₃Fe₂O₉]_m[Bi₄Sr₆Fe₂O₁₆] collapsed family. This new collapsed structure can be described as slices of 2212 structure of five bismuth polyhedra thick along , shifted with respect to each other and interconnected by means of [Bi₄Sr₆Fe₂O₁₆] slices. The latter are the place of numerous defects like iron or strontium for bismuth substitution; they can be correlated to intergrowth defects with other members of the family.     

Ion-beam irradiation of lanthanum compounds in the systems La2O3-Al2O3 and La2O3-TiO2

Thin crystals of La₂O₃, LaAlO₃, La_2/3TiO₃, La₂TiO₅, and La₂Ti₂O₇ have been irradiated in situ using 1 MeV Kr²⁺ ions at the Intermediate Voltage Electron Microscope-Tandem User Facility (IVEM-Tandem), Argonne National Laboratory (ANL). We observed that La₂O₃ remained crystalline to a fluence greater than 3.1×10¹⁶ ions cm⁻² at a temperature of 50 K. The four binary oxide compounds in the two systems were observed through the crystalline-amorphous transition as a function of ion fluence and temperature. Results from the ion irradiations give critical temperatures for amorphisation (T_c) of 647 K for LaAlO₃, 840 K for La₂Ti₂O₇, 865 K for La_2/3TiO₃, and 1027 K for La₂TiO₅. The T_c values observed in this study, together with previous data for Al₂O₃ and TiO₂, are discussed with reference to the melting points for the La₂O₃-Al₂O₃ and La₂O₃-TiO₂ systems and the different local environments within the four crystal structures. Results suggest that there is an observable inverse correlation between T_c and melting temperature (T_m) in the two systems. More complex relationships exist between T_c and crystal structure, with the stoichiometric perovskite LaAlO₃ being the most resistant to amorphisation.     

Crystal growth, structural characterization and magnetic properties of Ca3CuRhO6, Ca3Co1.34Rh0.66O6 and Ca3FeRhO6

Single crystals of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ were synthesized by high temperature flux growth in molten K₂CO₃ and structurally characterized by single crystal X-ray diffraction. While Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ crystallize with trigonal (rhombohedral) symmetry in the space group , Z=6: Ca₃Co_1.34Rh_0.66O₆a=9.161(1) Å, c=10.601(2) Å; Ca₃FeRhO₆a=9.1884(3) Å, c=10.7750(4) Å; Ca₃CuRhO₆ adopts a monoclinic distortion of the K₄CdCl₆ structure in the space group C2/c, Z=4: a=9.004(2) Å, b=9.218(2) Å, c=6.453(1) Å, β=91.672(5). All crystals of Ca₃CuRhO₆ examined were twinned by pseudo-merohedry. Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are structurally related and contain infinite one-dimensional chains of alternating face-sharing RhO₆ octahedra and MO₆ trigonal prisms. In the monoclinic modification, the copper atoms are displaced from the center of the trigonal prism toward one of the rectangular faces adopting a pseudo-square planar configuration. The magnetic properties of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are discussed.     

The mercury chromates Hg6Cr2O9 and Hg6Cr2O10—Preparation and crystal structures, and thermal behaviour of Hg6Cr2O9

The basic mercury(I) chromate(VI), Hg₆Cr₂O₉ (=2Hg₂CrO₄·Hg₂O), has been obtained under hydrothermal conditions (200 °C, 5 days) in the form of orange needles as a by-product from reacting elemental mercury and K₂Cr₂O₇. Hydrothermal treatment of microcrystalline Hg₆Cr₂O₉ in demineralised water at 200 °C for 3 days led to crystal growth of red crystals of the basic mercury(I, II) chromate(VI), Hg₆Cr₂O₁₀ (=2Hg₂CrO₄·2HgO). The crystal structures were solved and refined from single crystal X-ray data sets. Hg₆Cr₂O₉: space group P2₁2₁2₁, Z=4, a=7.3573(12), b=8.0336(13), , 3492 structure factors, 109 parameters, R[F²>2σ(F²)]=0.0371, wR(F² all)=0.0517; Hg₆Cr₂O₁₀: space group Pca2₁, Z=4, a=11.4745(15), b=9.4359(12), , 3249 structure factors, 114 parameters, R[F²>2σ(F²)]=0.0398, wR(F² all)=0.0625. Both crystal structures are made up of an intricate mercury-oxygen network, subdivided into single building blocks [O-Hg-Hg-O] for the mercurous compound, and [O-Hg-Hg-O] and [O-Hg-O] for the mixed-valent compound. Hg₆Cr₂O₉ contains three different Hg₂²⁺ dumbbells, whereas Hg₆Cr₂O₁₀ contains two different Hg₂²⁺ dumbbells and two Hg²⁺ cations. The Hg^I-Hg^I distances are characteristic and range between 2.5031(15) and 2.5286(9) Å. All Hg₂²⁺ groups exhibit an unsymmetrical oxygen environment. The oxygen coordination of the Hg²⁺ cations is nearly linear with two tightly bonded O atoms at distances around 2.07 Å. For both structures, the chromate(VI) anions reside in the vacancies of the Hg-O network and deviate only slightly from the ideal tetrahedral geometry with average Cr-O distances of ca. 1.66 Å. Upon heating at temperatures above 385 °C, Hg₆Cr₂O₉ decomposes in a four-step mechanism with Cr₂O₃ as the end-product at temperatures above 620 °C.     

LiNi0.8Co0.15Al0.05O2正极材料的FePO4包覆改性

使用液相包覆工艺对LiNi_(0.8)Co_(0.15)Al_(0.05)O_2(NCA)材料进行FePO_4包覆改性,利用FePO_4优异的结构稳定性与热稳定性,对NCA的长期可靠性与安全性能进行改良。重点研究FePO_4包覆对NCA材料的改性效果,以及不同包覆量造成的NCA材料电化学性能差异。表面包覆的FePO_4保护层,能够防止NCA材料与电解液直接接触发生副反应,抑制长期循环过程中过渡金属离子的溶出,保持结构的长期稳定性。当包覆量为1.0%(w/w)时,NCA材料表现出最优的综合性能,充放电循环800次后,容量保持率依然高达95%,25℃下存储100 d后,容量保持率也高于95%,达到了兼顾能量密度、使用寿命及安全性能的理想效果。     

Solubility of (UO2)3(PO4)2?4H2O in H+-Na+-OH?-H2PO?4-HPO2?4-PO3?4-H2O and Its Comparison to the Analogous PuO2 +2 System

The objectives of this study were to address uncertainties in the solubility product of (UO₂)₃(PO₄)₂⋅4H₂O(c) and in the phosphate complexes of U(VI), and more importantly to develop needed thermodynamic data for the Pu(VI)-phosphate system in order to ascertain the extent to which U(VI) and Pu(VI) behave in an analogous fashion. Thus studies were conducted on (UO₂)₃(PO₄)₂⋅4H₂O(c) and (PuO₂)₃(PO₄)₂⋅4H₂O(am) solubilities for long-equilibration periods (up to 870 days) in a wide range of pH values (2.5 to 10.5) at fixed phosphate concentrations of 0.001 and 0.01 M, and in a range of phosphate concentrations (0.0001–1.0 M) at fixed pH values of about 3.5. A combination of techniques (XRD, DTA/TG, XAS, and thermodynamic analyses) was used to characterize the reaction products. The U(VI)-phosphate data for the most part agree closely with thermodynamic data presented in Guillaumont et al.,⁽¹⁾ although we cannot verify the existence of several U(VI) hydrolyses and phosphate species and we find the reported value for formation constant of UO₂PO⁻₄ is in error by more than two orders of magnitude. A comprehensive thermodynamic model for (PuO₂)₃(PO₄)₂⋅4H₂O(am) solubility in the H⁺-Na⁺-OH⁻-Cl⁻-H₂PO⁻₄-HPO²⁻₄-PO³⁻₄-H₂O system, previously unavailable, is presented and the data shows that the U(VI)-phosphate system is an excellent analog for the Pu(VI)-phosphate system.