La1－xSrxNi1－yFeyO3型钙钛矿双功能氧电极的电化学性能研究

采用溶胶-凝胶法制备了一系列La_1－xSr_xNi_1－yFe_yO₃ (x＝0, 0.1, 0.2, 0.5; y＝0～1.0)型的钙钛矿催化剂, 以活性碳为载体, PTFE乳液为粘接剂制备双功能氧电极. 对催化剂进行了XRD结构分析以及SEM分析和BET比表面积测量. 采用三电极体系测试了氧电极的稳态极化曲线和电化学交流阻抗谱并对其阴极极化和阳极极化的交流阻抗谱图进行分析. 通过等效电路的拟合研究了该系列双功能氧电极氧还原反应的工作机理. 实验表明对于LaNiO₃化合物, B位掺杂可显著提高催化剂的电催化性能; 电极氧还原反应的极化主要由电荷转移反应和Nernstian扩散过程造成. 通过各个电极对于催化分解H₂O₂的分解速率常数的测定得知, Ni离子对于催化H₂O₂分解反应的活性大于Fe离子, 继续在对于氧还原反应和氧析出反应都具有较高电催化活性的LaNi_0.8Fe_0.2O₃催化剂上进行A位掺杂Sr离子后显著提高了催化剂分解H₂O₂的催化活性, 主要是因为氧空位的增多和金属离子d电子含量的降低有利于催化分解H₂O₂的活性的提高, 但由于氧空位的增多导致催化剂电导率的降低, 所以其电催化活性降低了. 通过多圈循环伏安扫描的测试, 催化剂LaNi_0.8Fe_0.2O₃有很好的稳定性.     

La1－xSrxNi1－yFeyO3型钙钛矿双功能氧电极的电化学性能研究

采用溶胶-凝胶法制备了一系列La_1－xSr_xNi_1－yFe_yO₃ (x＝0, 0.1, 0.2, 0.5; y＝0～1.0)型的钙钛矿催化剂, 以活性碳为载体, PTFE乳液为粘接剂制备双功能氧电极. 对催化剂进行了XRD结构分析以及SEM分析和BET比表面积测量. 采用三电极体系测试了氧电极的稳态极化曲线和电化学交流阻抗谱并对其阴极极化和阳极极化的交流阻抗谱图进行分析. 通过等效电路的拟合研究了该系列双功能氧电极氧还原反应的工作机理. 实验表明对于LaNiO₃化合物, B位掺杂可显著提高催化剂的电催化性能; 电极氧还原反应的极化主要由电荷转移反应和Nernstian扩散过程造成. 通过各个电极对于催化分解H₂O₂的分解速率常数的测定得知, Ni离子对于催化H₂O₂分解反应的活性大于Fe离子, 继续在对于氧还原反应和氧析出反应都具有较高电催化活性的LaNi_0.8Fe_0.2O₃催化剂上进行A位掺杂Sr离子后显著提高了催化剂分解H₂O₂的催化活性, 主要是因为氧空位的增多和金属离子d电子含量的降低有利于催化分解H₂O₂的活性的提高, 但由于氧空位的增多导致催化剂电导率的降低, 所以其电催化活性降低了. 通过多圈循环伏安扫描的测试, 催化剂LaNi_0.8Fe_0.2O₃有很好的稳定性.     

乙烷部分氧化超细Fe－Mo－O催化剂的研究

采用溶胶-凝胶法制备了Fe－Mo－O催化剂，用XRD、TEM、BET、IR、TPR、TPD和微反等技术研究了催化剂晶体结构、表面构造、晶格氧活泼性、化学吸附和乙烷部分氧化反应性能。Fe－Mo－O复合氧化物催化剂是由超细微粒组成，微粒粒径约10 nm～20 nm，比表面积为48.1 m2/g。催化剂表面由Lewis碱位（Mo=O键的端氧和Fe－O－Mo键中的桥氧）及Lewis酸位构成。乙烷能以甲基中的H原子吸附在催化剂表面Lewis碱位Mo=O的端氧上形成分子吸附态，其部分氧化产物主要是C2H4和少量的CH3CHO。     

MoO3/SiO2催化剂的异丁烷选择氧化反应性能

分别采用浸渍法和溶胶－凝胶法制备了MoO3/SiO2催化剂，用XRD，TPR，IR，TPD和活性评价等手段对催化剂的影响，晶格氧活泼性，化学吸附性能和异丁烷选择氧化反应性能进行了研究。结果表明，催化剂表面由Lewis碱位Mo=M,Mo-O-Mo中的晶格氧和Lewis酸位Mo^6 构成，在MoO3/SiO2催化剂上，异丁烷主要通过甲基的H双位吸附在表面的Lewis碱位Mo=O上；在常压条件下，异丁烷选择氧化产物主要为异丁烷，甲基丙烯醛和甲基丙烯酸，其中深度氧化产物CO2主要由吸附的异丁烯继续反应生成；采用溶胶－凝胶法制备的MoO3/SiO2催化剂，可得到较高的异丁烷转化率和含氧有机物选择性。     

Mo-P-O/SiO2催化剂上的异丁烷选择氧化反应

 采用溶胶－凝胶法制备了MoO3／SiO2和Mo－P－O／SiO2催化剂，用X射线衍射、红外光谱、程序升温还原、程序升温脱附和活性评价等手段研究了催化剂的表面结构、晶格氧活泼性、化学吸附性能以及异丁烷选择氧化反应性能．结果表明，活性组分在催化剂表面分散较好；异丁烷吸附在催化剂表面Lewis碱位的MoO端氧上形成分子吸附态；MoO3／SiO2和Mo－P－O／SiO2两种催化剂对异丁烷选择氧化都有较好的选择性，将PO3－4引入到MoO3／SiO2催化剂中可提高含氧化合物的选择性     

镓掺杂SO2－4／ZrO2的制备及其对正丁烷异构化反应的催化性能

 通过沉淀、回流和浸渍法制备了镓掺杂的纳米级固体超强酸SO2－4／Ga2O3／ZrO2，并用X射线衍射、透射电镜、热重、吡啶吸附红外光谱、低温N2－BET及化学分析等技术对SO2－4／Ga2O3／ZrO2的结构、表面性质及其对正丁烷异构化反应的催化活性进行了研究．结果表明，掺杂Ga2O3可以抑制制备过程中ZrO2晶粒长大，有利于抑制高温下催化剂由四方相转变为单斜相．与未掺杂的催化剂相比，Ga2O3的掺杂提高了催化剂表面SO2－4的分解温度，有利于催化剂表面形成更多的酸中心．SO2－4／Ga2O3／ZrO2对正丁烷异构化反应显示出优异的催化性能．其中，含3％Ga2O3的样品的活性最高，220℃下其初活性为59．1％；反应1h后，其活性基本保持稳定，稳态转化率大于51％，接近该反应条件下正丁烷的平衡转化率．     

掺杂对Pd/Al2O3催化剂物相结构及表面氧性质的影响

采用XRD、DTA、TPD－MS及流动反应法等手段，研究了掺杂超细ZrO2对Pd／Al2O3催化剂物相结构、表面氧性能及催化活性的影响.结果表明，掺杂超细ZrO2，对催化剂Pd／Al2O3的载体物相变化（α－Al2O3的生成）有明显的抑制作用，很高了催化剂的贮氧能力及表面吸附氧的活性，从而提高了催化剂的耐热稳定性、氧化能力以及对贫氧气氛的适应能力．     

钕掺杂Ti基Sn-Sb涂层电极的制备及性能评价

以SnCl4·5H2O, Sb2O3和Nd(NO3)3·6H2O为前驱体, 纯钛板为基体, 采用涂层热解法制备了Nd掺杂Ti基Sn-Sb氧化物涂层电极. 通过对所制备电极的析氧电位和含阴离子表面活性剂污水降解效果的考察, 优化出最佳Nd掺杂量为SnSbNd=10062.5(摩尔比), 最佳热处理温度为550 ℃. 通过SEM, XRD和EDX等检测手段对制备的电极的表面形貌、晶体结构及元素组成进行了表征和分析, 结果证明, 适量Nd的掺杂使Ti/Sn-Sb电极的析氧电位明显提高, 达到1.72 V, 对阴离子表面活性剂的去除率达到97.4%, 使电极表面晶粒细化, 对基体覆盖较好. 掺杂过量会使SnO2晶格破坏, 使电极性能降低, 甚至低于未掺杂电极.     

乙烷部分氧化制C2氧化物用Fe－Al－P－O催化剂的研究Ⅰ．超细Fe－Al－P－O催化剂的制备与表征

 用溶胶－凝胶法制备了超细Fe－Al－P－O催化剂，并用DTA－TG，BET，TEM，XRD，TPR和IR等技术研究了催化剂的微观组成和结构及其晶格氧活性，探讨了催化剂的制备工艺，考察了溶胶－凝胶的形成机理、凝胶干燥及焙烧条件对催化剂微观组成和结构的影响规律．结果表明，Fe－Al－P－O催化剂呈非晶态，是具有均匀分布的超细粒子（10nm），其比表面积大（238m2／g），晶格氧活性高．FePO4和AlPO4间隔分布在催化剂表面，形成Lewis碱位（P＝O，P－O－Fe）和Lewis酸位（Fe3＋，Al3＋）．     

铽氧化物电极表面的XPS和电化学循环伏安分析

以热分解工艺制备铽氧化物电极，采用ＸＰＳ和电化学循环２伏安法分析铽氧化物的表面特征和在７００℃高温ＮａＣｌ－ＫＣｌ熔体中析氯过程的行为。ＸＰＳ分析表明，热分解产物表面成分为非化学计量，有结构缺陷的混合价态铽的氧化物；电极表面的循环极化反应映出Ｃｌ＾－的特性吸附和电解质中电极表面结构变化过程；循环伏安分析揭示了表面氧化物的氧化还原行为及在电催化过程中的作用。通过测定循环伏安电量研究电催化剂制备时温度     

Pr1-xSrCo0.5Ni0.5O4+δ阴极材料的合成及电化学性质

采用固相法合成中温固体氧化物燃料电池(IT-SOFC)阴极材料Pr_(1-x)SrCo_(0.5)Ni_(0.5)O_(4+δ)(P_(1-x)SCN,x=0.00,0.05,0.10,0.15,0.20),并对材料的物相、热膨胀系数(TEC)、电导率、电极的微观形貌以及电化学性质进行表征。XRD结果表明,该材料形成单一的K_2NiF_4结构,空间群为I4/mmm,并与电解质材料Ce_(0.9)Gd_(0.1)O_(1.95)(CGO)具有良好的高温化学相容性。碘量法分析表明随着Pr离子缺位浓度增加,P_(1-x)SCN中Co/Ni离子平均化合价随着x的增加而升高,至x=0.10后逐渐降低,而氧空位含量逐渐升高。引入Pr离子缺位使材料的电导率明显提高,其中P_(0.90)SCN在700℃空气中电导率值为309 S·cm~(-1)。TEC测试结果显示,随着Pr缺位的增加,热膨胀系数逐渐增大,最大值为1.51×10~(-5)K~(-1)。交流阻抗谱(EIS)测试结果表明,Pr缺位明显降低了电极的极化阻抗值,P_(0.90)SCN阴极在700℃空气中的极化阻抗值为0.21Ω·cm~2。电解质支撑NiO-CGO/CGO/P_(0.90)SCN单电池在700℃最大输出功率密度为197.8 mW·cm~(-2)。     

Influence of vacancy ordering on the percolative behavior of (Li(1)(-x)Na(x))(3y)La(2/3-y)TiO(3) perovskites

Influence of the vacancy concentration on the Li conductivity of the (Li(1-x)Na(x))(0.2)La(0.6)TiO(3) and (Li(1-x)Na(x)(0.5)La(0.5)TiO(3) perovskite series, with 0 < or = x < 1, has been investigated by neutron diffraction (ND), impedance spectroscopy (IS), nuclear magnetic resonance (NMR), and Monte Carlo simulations. In both series, Li(+) ions occupy unit cell faces, but Na(+) ions are located at A sites of the perovskite. From this fact, the amount of vacant A sites that participate in Li conductivity is given by the expression n(v) = [Li] + square, where square is the nominal vacancy concentration. Substitution of Li by Na decreases the amount of vacancies, reducing drastically the Li conductivity when n(v) approaches the percolation threshold of the perovskite conduction network. In disordered (Li(1-x)Na(x))(0.5)La(0.5)TiO(3) perovskites, the percolation threshold is 0.31; however, in ordered (Li(1-x)Na(x))(0.2)La(0.6)TiO(3) perovskites, this parameter changes to 0.26. Near the percolation threshold, the amount of mobile Li species deduced by (7)Li NMR spectroscopy is lower than that derived from structural formulas but higher than deduced from dc conductivity measurements. Conductivity values have been explained by Monte Carlo simulations, which assume a random walk for Li ions in the conduction network of the perovskite. In these simulations, distribution of vacancies conforms to structural models deduced from ND experiments.     

Ce1-xMnxO2表面性质对催化CO2和甲醇直接合成DMC反应活性的影响

通过共沉淀法制备了一系列Mn掺杂量不同的Ce_1-xMn_xO₂催化剂, 并将其用于催化CO₂和甲醇直接合成碳酸二甲酯(DMC). 通过X射线衍射(XRD)、 氮气吸附-脱附、 透射电子显微镜(TEM)、 X射线光电子能谱(XPS)和程序升温脱附(TPD)等手段研究了Ce_1-xMn_xO₂表面性质对催化CO₂和甲醇直接合成DMC反应活性的影响. 结果表明, Mn离子进入CeO₂晶格中形成固溶体, 随着Mn掺杂量增加, 催化剂表面弱酸碱位数量逐渐降低, 中强酸碱和强酸碱位数量增加, 催化剂表面氧空位含量呈先增加后减少的变化趋势, 当Mn掺杂量较少时, 催化剂表面Mn²⁺比例较高, 有利于Ce⁴⁺+Mn²⁺→Ce³⁺+Mn³⁺反应的进行, 促进催化剂表面氧空位生成; 进一步提高Mn掺杂量时, 催化剂表面Mn⁴⁺比例提高, 有利于Ce³⁺+Mn⁴⁺→Ce⁴⁺+Mn³⁺反应的进行, 导致催化剂表面氧空位含量减少. 研究发现Ce_1-xMn_xO₂催化剂活性与表面氧空位含量线性相关.     

Perovskite Oxides La0.8Sr0.2Co1-xFexO3 for CO Oxidation and CO+NO Reduction: Effect of Redox Property and Surface Morphology

This work aims to study the effect of redox property and surface morphology of perovskite oxides on the catalytic activity of CO oxidation and CO+NO reduction, with the redox property being tuned by doping Fe at the Co site of La_0.8Sr_0.2Co_1-xFe_xO₃ and the surface morphology being modified by supporting La_0.8Sr_0.2CoO₃ on various mesoporous silicas(i.e., SBA-16, SBA-15, MCF). Characteristic results show that the Fe doping improves the match of redox potentials, and SBA-16 is the best support of La_0.8Sr_0.2CoO₃ when referring to the oxidation ability(e.g., the Co³⁺/Co²⁺ molar ratio). A mechanism for oxygen desorption from perovskite oxides is proposed based on O₂-TPD experiments, showing the evolution process of oxygen released from oxygen vacancy and lattice framework. Catalytic tests indicate that La_0.8Sr_0.2CoO₃ is the best for CO oxidation, and La_0.8Sr_0.2FeO₃ is the best for CO+NO reduction. The mechanism of CO+NO reduction changes as the reaction temperature increases, with X_NO/X_CO value decreases from 2.4 at 250 ℃ to 1.0 at 400 ℃. As for the surface morphology, La_0.8Sr_0.2CoO₃ supported on SBA-16 possesses the highest surface Co³⁺/Co²⁺ molar ratio as compared to the other two, and shows the best activity for CO oxidation.     

Mixed conductivity, nonstoichiometric oxygen, and oxygen permeation properties in Co-Doped Sr3Ti2O(7-δ)

Electrical conductivity and oxygen permeation rates in Co-doped Sr(3)Ti(2)O(7-δ) with Ruddesden-Popper type structures were investigated. The effects of metal dopants (M) in the Ti site of Sr(3)Ti(2)(M)O(7-δ) on the mixed conductivity were also studied. Doping of Sr(3)Ti(2)O(7-δ) with Co was found to be effective for improving the electrical conductivity as well as the oxygen permeation rate, which could be assigned to the increased oxygen vacancy concentration by doping Co(3+) into Ti(4+) sites. The nonstoichiometric oxygen of these oxides was measured by using a thermal gravimetric method. The creation of oxygen vacancies, which is compensated with Co(3+) doping, leads to higher oxide ion conductivity. The oxygen permeation rate monotonously increased with increasing amounts of Co in the Ti site. Sr(3)Ti(0.8)Co(1.2)O(7-δ) exhibited high oxide ion conductivity and a large oxygen permeation rate. The highest oxygen permeation rate achieved a value of 2.02 cc min(-1) cm(-2) at 1273 K for Sr(3)Ti(0.8)Co(1.2)O(7-δ). Neutron diffraction analysis and redox titration suggests that the oxygen diffusion occurs through oxygen vacancies in the perovskite block, but not through excess oxygen in the rock salt block.     

Defect and dopant properties of the Aurivillius phase Bi4Ti3O12

Computer modelling techniques have been used to investigate the defect and oxygen transport properties of the Aurivillius phase Bi₄Ti₃O₁₂. A range of cation dopant substitutions has been considered including the incorporation of trivalent ions (M³⁺=Al, Ga and In). The substitution of In³⁺ onto the Bi site in the [Bi₂O₂] layer is predicted to be the most favourable. The calculations suggest that lanthanide (Ln³⁺) doping at the dilute limit preferentially occurs in the [Bi₂O₂] layer, with probable distribution over both the [Bi₂O₂] and the perovskite A-site at higher dopant levels. It is predicted that the reduction process involving Ti³⁺ and oxygen vacancy formation is energetically favourable. The energetics of oxide vacancy migration between various oxygen sites in the structure have been investigated.     

Electrochemical impedance spectroscopy of mixed conductors under a chemical potential gradient: a case study of Pt|SDC|BSCF

The AC impedance response of mixed ionic and electronic conductors (MIECs) exposed to a chemical potential gradient is derived from first principles. In such a system, the chemical potential gradient induces a gradient in the carrier concentration. For the particular system considered, 15% samarium doped ceria (SDC15) with Ba(0.5)Sr(0.5)Co(0.8)Fe(0.2)O(3-delta) (BSCF) and Pt electrodes, the oxygen vacancy concentration is a constant under the experimental conditions and it is the electron concentration that varies. The resulting equations are mapped to an equivalent circuit that bears some resemblance to recently discussed equivalent circuit models for MIECs under uniform chemical potential conditions, but differs in that active elements, specifically, voltage-controlled current sources, occur. It is shown that from a combination of open circuit voltage measurements and AC impedance spectroscopy, it is possible to use this model to determine the oxygen partial pressure drop that occurs between the gas phase in the electrode chambers and the electrode|electrolyte interface, as well as the interfacial polarization resistance. As discussed in detail, this resistance corresponds to the slope of the interfacial polarization curve. Measurements were carried out at temperatures between 550 and 650 degrees C and oxygen partial pressure at the Pt anode ranging from 10(-29) to 10(-24) atm (attained using H(2)/H(2)O/Ar mixtures), while the cathode was exposed to either synthetic air or neat oxygen. The oxygen partial pressure drop at the anode was typically about five orders of magnitude, whereas that at the cathode was about 0.1 atm for measurements using air. Accordingly, the poor activity of the anode is responsible for a loss in open circuit voltage of about 0.22 V, whereas the cathode is responsible for only about 0.01 V, reflecting the high activity of BSCF for oxygen electro-reduction. The interfacial polarization resistance at the anode displayed dependences on oxygen partial pressure and on temperature that mimic those of the electronic resistivity of SDC15. This behavior is consistent with hydrogen electro-oxidation occurring directly on the ceria surface and electron migration being the rate-limiting step. However, the equivalent resistance implied by the oxygen partial pressure drop across the anode displayed slightly different behavior, possibly indicative of a more complex reaction pathway.     

Kinetic Monte Carlo simulations of oxygen vacancy diffusion in a solid electrolyte: Computing the electrical impedance using the fluctuation–dissipation theorem

We present a new method for computing the electrical impedance of solid oxide electrolyte from kinetic Monte Carlo simulations of oxygen vacancy diffusion. The impedance values at all frequencies are obtained from a single equilibrium simulation based on the fluctuation–dissipation theorem, leading to a significant gain of efficiency over existing methods.This allows us to systematically examine the effect of dopant concentration. Increasing dopant concentration is found to decrease the infinite-frequency impedance, which is attributed to the increasing density of oxygen vacancies. The difference between the impedance values at zero- and infinite-frequency, on the other hand, shows the opposite trend, and is linked to dopant–vacancy interactions. Hence the two competing mechanisms, previously proposed to explain the existence of an optimal doping concentration, are separately quantified.Our model also predicts a significant effect of the arrangement of dopant cations on the electrolyte conductivity.     

高性能Sm0.5Sr0.5CoO3阴极的制备与表征

用固相合成法合成了Sm0.5Sr0.5CoO3 (SSC)中温固体氧化物燃料电池阴极材料.以La0.9Sr0.1Ga0.8Mg0.2O3为电解质,利用多种技术考察了不同温度(1173～1373 K)焙烧的SSC阴极,以及1173 K 焙烧、掺杂La0.8Sr0.2Ga0.8Mg0.15Co0.05O3(LSGMC5)或La0.8Sr0.2Ga0.8Mg0.09Co0.11O3 (LSGMC11)高氧离子电导材料的复合SSC阴极.SEM的结果显示,随着电极焙烧温度的增加,电极的颗粒度增大,孔隙度减小；LSGMC5、LSGMC11的掺杂对电极微观结构影响不大.交流阻抗和极化实验的结果表明,SSC电极的活性随电极焙烧温度的增加而减小,电极的最佳焙烧温度在1173 K左右；掺杂了LSGMC5或LSGMC11的复合SSC电极的活性以及稳定性显著高于SSC电极.