改性LiClO_4－（PEO）_（20）电解质锂离子迁移数的测定

采用交流阻抗和恒电位计时电流法测定了ＬｉＣｌＯ４·（ＰＥＯ）２０·（ＰＣ）１２·（ＥＣ）１２高分子电解质的锂离子迁移数。在非水溶液和高分子电解质中,锂是热力学不稳定的,表面生成一层固体电解质钝化膜,严重地影响了锂离子迁移数的准确测定。本方法避免固体电解质钝化膜的影响,给出正确的锂离子迁移数测定值,实验表明,ＬｉＣｌＯ４·（ＰＥＯ）２０·（ＰＣ）１２·（ＥＣ）１２电解质的电导率为０．８×１０－３／ｃｍ,锂离子迁移数为０．３。     

微管式固体氧化物燃料电池电解质膜的制备

基于聚合物溶液相分离诱导原理提出了一种新的微管式固体氧化物燃料电池（SOFC）电解质膜制备方法,应用该方法制得了YSZ电解质微管膜,该膜由致密电解质薄层和可制成电极的多孔层组成,其中YSZ致密电解质膜和多孔层厚度分别为3～5μm和70-90μm,而多孔层内表面孔隙率高于28．1％,电解质层和多孔层之间结合紧密,可避免电解质膜开裂或剥落等导致的电池性能降低等问题．该方法具有工艺简单、成本低、可靠性好等优点,为微管式SOFC电解质膜及电池的制备提供了一条新的途径．     

锂离子电池负极碳材料的表面改性与修饰 Ⅲ.人工施加的固体电解质膜对锂碳负极电池性能的改善

研究了人工施加的无机固体电解质晶体膜对锂碳负极电池性能的影响作用,结果表明碳电极的容量及首次充放电效率相对于未改性电极都得到了一定程度的提高,显示了以这层外界人工施加的晶体膜替代由电极体系本身所形成的钝化膜之有效性．扫描电子显微镜的研究直观地显示了这层人工施加膜的均匀、致密性质．     

锂离子电池负极碳材料的表面改性与修饰：Ⅲ,人工施加的固体电解质膜…

研究了人工施加的无机固体电解质体膜对锂碳负极电池性能的影响作用，结果表明碳电极的容量及首次充放电效率相对于未改性电极都得到了一定程度的提高。显示了以这层外界人工施加的晶体膜替代的电极体系本身所形成的钝化膜之有效性，扫描电子显微镜的研究直观地显示了这层人工施加膜的均匀，致密性质。     

基于高度非对称结构电解质中空纤维的微管式固体氧化物燃料电池制备

提出了一种简单而方便的微管式固体氧化物燃料电池(MT-SOFCs)的制备新方法.首先应用改进相转化-烧结技术制备由致密电解质表皮薄层和多孔支撑层构成的高度非对称结构电解质中空纤维膜(微管),在电解质中空纤维膜的多孔支撑层内通过化学镀法沉积Ni催化剂作为电池阳极,而致密电解质表皮层直接作为电解质膜,在电解质微管外表面用浆料涂层法制备电池的多孔阴极,烧结后即得到完整的MT-SOFC.应用该方法制备了Ni-YSZ|YSZ|LSCF微管式电池,该电池以H2/空气作原料气,在800℃时最大输出功率达到159.6mWcm-2.     

炔醇类缓蚀剂对铁在硫酸溶液中保护作用的光电化学研究

在含不同缓蚀剂的0．5mol/L H2SO4的电解质溶液中,用光电化学方法研究了氧化铁钝化膜的电子传递过程;缓蚀剂的加入在金属表面形成的沉积膜是非光电化学活性的,基本上对光电流的瞬态性质不造成影响;在硫酸溶液中测得两个明显的光电流峰,其禁带宽度值Eg^dir=3.7eV(对应300nm处的弱峰）,Eg^ind=1.95eV(380到500nm范围的强峰）,加入不同缓蚀剂后测得Eg^ind值略有减小;测定电位阶跃下发生的电流瞬态引起电荷量的改变,表明在恒定电位下延长钝化时间会减少膜中羟量和水的含量,而缓蚀剂的加入减少了膜中OH^-和H2O的含量,说明缓蚀剂沉积膜与钝化膜之间存在着化学作用,造成了钝化膜表面附近的化学组成发生变化。     

液态Wood合金在NaOH电解质溶液中的电毛细变形现象

本文研究了液态Wood合金在氢氧化钠电解质溶液中,通过施加外电场,进而诱发液态金属电毛细变形的现象. 当石墨电极伸入金属液滴内部时,通电后在金属表面发生的电极反应,促使金属表面形成氧化膜或去除氧化膜. 由于氧化膜与液态金属的表面张力存在巨大差异,通电后电极极性的变化可实现金属液滴形状的快速可逆变形.在液态金属与电解质溶液之间形成的双电子层中,当两侧聚集同极性电荷时将降低界面张力.为维持通电后体系自由能最小,将迫使液体金属增大与溶液之间的界面面积,在宏观上表现为液体金属的变形,由于液态金属与氢氧化钠反应后自身携带负电荷,在电场力的作用下可有效地驱动液态金属在电解质溶液中的运动.     

液态Wood合金在氢氧化钠电解质溶液中的电毛细变形现象

本文研究了液态Wood合金在氢氧化钠电解质溶液中,通过施加外电场,进而诱发液态金属电毛细变形的现象.当石墨电极伸入金属液滴内部时,通电后在金属表面发生的电极反应,促使金属表面形成氧化膜或去除氧化膜.由于氧化膜与液态金属的表面张力存在巨大差异,通电后电极极性的变化可实现金属液滴形状的快速可逆变形.在液态金属与电解质溶液之间形成的双电子层中,当两侧聚集同极性电荷时将降低界面张力.为维持通电后体系自由能最小,将迫使液体金属增大与溶液之间的界面面积,在宏观上表现为液体金属的变形,由于液态金属与氢氧化钠反应后自身携带负电荷,在电场力的作用下可有效地驱动液态金属在电解质溶液中的运动.     

缓蚀剂对船用钢在潮湿大气中的防蚀研究

模拟 90 7A钢在海水的潮湿大气环境和表面覆有薄层缓蚀剂液膜状态下其腐蚀受抑制的情况 ,利用恒电量仪连接ACM控头 ,监测其腐蚀状态 ,结合电化学阻抗谱 (EIS)的测量 ,探讨 90 7A钢在薄层缓蚀剂液膜下的腐蚀受到抑制机理 .结果表明 :此时大气腐蚀反应已转变为阳极过程控制占优势 ,在浸润后期的EIS呈现出由腐蚀介质扩散和电化学放电混合控制特征 ,如果利用恒电量激励下的等效电路模型解析 ,则可以更清楚地获知薄层缓蚀剂液膜下金属表面膜层的信息     

原位聚合法制备凝胶型离子液体／PMMA聚合物电解质

采用原位聚合法制备了含有N-甲基、丙基哌啶双三氟甲磺酰亚胺离子液体的凝胶型聚合物电解质．利用SEM和XPS测试了电解质膜与LiFePO4电极的界面状态,充放电循环后,在电解质膜与LiFePO4之间有一层薄膜,这层薄膜中含有N和S元素．结果表明,随着充放电的不断进行,凝胶型电解质中未聚合的甲基丙烯酸甲酯与电极表面的锂离子之间发生电子转移,形成SEI膜,至少要三个循环后才能形成稳定的SEI膜．随着SEI膜的增厚,放电容量增加,阻碍了电子转移,使系统更加的稳定．在不同倍率下测试了凝胶型离子液体／PMMA聚合物电解质电池性能,当充放电达到30个循环时,0．2、0．5和1C下电池比容量分别为132、128和120mAh／g．     

Formal Mathematical Analysis of the Existence of the Common Intersection Point in Relation to Determining the Parameters Describing Ion Adsorption at the Oxide/Electrolyte Interface: Comparison of the Triple and Four-Layer Models

For most oxide/electrolyte systems potentiometric titration curves measured for different ionic strengths have a Common Intersection Point (CIP) which corresponds to the Point of Zero Charge (PZC). However, there are systems where a CIP exists but the surface charge at this point does not equal zero (PZC CIP). In this paper theoretical analysis of the systems in which the PZC and CIP do not coincide is presented. It is based on the well-known 2-pK surface charging approach and Triple Layer Model (TLM) as well as the Four Layer Model (FLM) of the electric double layer. The appropriate mathematical criterion for CIP existence was applied with detailed derivations, both for TLM and FLM. Having determined in this manner the parameter values, one can draw proper conclusions about the features of oxide/electrolyte adsorption systems, in which PZC and CIP do not coincide. The values of adsorption parameters are found by fitting simultaneously the obtained theoretical expressions to both of the experimental titration isotherms, and to the individual isotherms of electrolyte cation adsorption measured using radiometric methods.     

First-principles simulations of the electrode|electrolyte interface

We review a direct dynamics method for the simulation of metal|water interfaces. The occupancy of on-top binding sites for water in this model as applied to a (100) surface of ‘copper' is very sensitive to potential. We suggest that this may account for some previously unexplained features of X-ray data on water structure and noble metal|water interfaces. We discuss the problem of statistical fluctuations on the occupancy of such tightly bound water molecules in such simulations. Though the problem is not too serious for charged interfaces, the problem of accounting for fluctuations at zero charge can be quite formidable, as we illustrate for the (100) surface of copper.     

Recent Advances in Gas Barrier Thin Films via Layer‐by‐Layer Assembly of Polymers and Platelets

Layer‐by‐layer (LbL) assembly has emerged as the leading non‐vacuum technology for the fabrication of transparent, super gas barrier films. The super gas barrier performance of LbL deposited films has been demonstrated in numerous studies, with a variety of polyelectrolytes, to rival that of metal and metal oxide‐based barrier films. This Feature Article is a mini‐review of LbL‐based multilayer thin films with a ‘nanobrick wall’ microstructure comprising polymeric mortar and nano­platelet bricks that impart high gas barrier to otherwise permeable polymer substrates. These transparent, water‐based thin films exhibit oxygen transmission rates below 5 × 10^‐3 cm³ m^‐2 day^‐1 atm^‐1 and lower permeability than any other barrier material reported. In an effort to put this technology in the proper context, incumbent technologies such as metallized plastics, metal oxides, and flake‐filled polymers are briefly reviewed.

     

Oxide density distribution across the barrier layer during the steady state growth of porous anodic alumina films: chronopotentiometry, kinetics of mass and thickness evolution and a high field ionic migration model

The steady state growth of porous anodic alumina films in oxalate solutions at various conditions was studied by chronopotentiometry, mass balance and optical microscopy methods enabling determination of consumed Al, film mass and thickness, current efficiencies, Al³⁺ and O²⁻ transport numbers across barrier layer, etc. The film thickness growth rate was found to be proportional to O²⁻ anionic current. A high field ionic migration model was developed. It predicted that, during anodising, the local oxide density across barrier layer rises from 2.6 in Al|oxide to 4.59–5.22 g cm⁻³ in oxide|electrolyte interface with mean value ≈3.21–3.52 g cm⁻³. The field strength rises from the first to second interface. The mechanism of Al oxidation near the Al|oxide interface embraces the transformation of the Al lattice to a transient, rare oxide one sustained by field with comparable Al³⁺ spacing parameter. The oxide near the Al|oxide interface and around the density maximum in the oxide|electrolyte interface are under different levels of electro-restriction stresses. During relaxation, the oxide behaves like a solid-fluid material suppressing the initial density distribution.     

Dissolution behavior of anodic oxide films formed in sulfanic acid on aluminum

Chemical dissolution of the barrier layer of porous oxide films formed on an aluminum foil (99.5% purity) in 1.5 M sulfanic acid after immersion in a 2 mol dm⁻³ sulphuric acid at 50 °C was studied. The barrier layer thickness before and after dissolution was determined using a re-anodizing technique. Re-anodizing was conducted in 0.5 mol dm⁻³ H³BO³/0.05 mol dm⁻³ Na²B⁴O⁷ solution. We found that the change in the porous oxide growth mechanism was observed at the anodizing voltage of 30 V. Taking into account this result chemical dissolution behaviour of the barrier layer of porous films formed at 20 V and 36 V and also the influence of annealing of oxide films at 200 °C were studied. We showed the interplay between the dissolution rates and charge distribution across the barrier layer. We conclude that the outer and middle layers have negative space charges and the inner layer has positive space charges.     

十八烷基胺在铁上成膜结构和耐腐蚀性研究

十八烷基胺(ODA)应用于热力设备停用保护技术在国外开发较早[1－3],国内电厂这二年来应用该技术也日益增多,但由于基础研究做得较少,使用效果受到影响.1996年以来我们对ODA的成膜条件和机理进行了一些研究[4－6],本文利用交流阻抗、俄歇电子能谱、红外镜反射光谱、光电化学等方法对ODA的成膜结构和耐蚀性进行探讨,同时介绍ODA在电厂的应用情况.1实验实验材料为DT-4型纯铁.样品制备及交流阻抗测试见文献[4－6].　　俄歇能谱(AES)Perkin-ElmerPHI550ESCA/SAM.实验在机械工业部上海材料研究所进行.　　红外镜反射(SR)Bio-R…     

Synergistic effect of water layer and divalent metal ions in a model oil sand on bitumen liberation from solids surface

In this work, we offer a direct evidence to illustrate the synergistic effect of water layer and divalent metal ions in oil sands on bitumen liberation from solids surface. A model oil sand was constructed by coating bitumen on the glass surface with a water layer containing divalent metal ions inserted between them. The bitumen liberation behaviors were investigated by placing the model oil sands in various pH solutions. It was found that the water layer facilitated the bitumen liberation, while the presence of Ca²⁺ or Mg²⁺ in the water layer played a different role on the bitumen liberation depending on the solution pH. It was believed that the variation of the bitumen liberation was attributed to the changes of surface wettability arising from the adsorption of natural surfactants on the solids and bitumen surfaces. The preferential adsorption of Ca²⁺ or Mg²⁺ on the solids and bitumen surfaces acted as either a barrier to disturb the cationic surfactants adsorbing or a bridge to anchor the anionic surfactants. The findings in this work are important for understanding the bitumen liberation behaviors and give a guideline of how controlling the water chemistry when processing the oil sands by water-based bitumen extraction processes.     

Effect of ac electrodeposition conditions on the growth of high aspect ratio copper nanowires in porous aluminum oxide templates

The effect of several deposition parameters on the uniformity of copper electrodeposition through the alumina barrier layer into porous aluminum oxide templates grown in sulfuric or oxalic acid was systematically investigated. A fractional factorial design of experiment was conducted to find suitable deposition conditions among the variables: frequency, voltage, pulsed or continuous deposition, electrolyte concentration, and barrier layer thinning voltage. Continuous ac sine wave deposition conditions yielded excellent uniformity of pore-filling but damaged the porous aluminum oxide templates when deposition was continued to grow bulk copper on the surface. Pulsed electrodeposition yielded comparable uniformity of pore-filling and no damage to the porous aluminum oxide templates, even when bulk copper was deposited on them. Further optimization of pulsed deposition conditions was accomplished by comparing square and sine waveforms and pulse polarity. Pulsed square waveforms produced better pore-filling than pulsed sine waveforms. For sine wave depositions, the oxidative/reductive pulse polarity was more efficient than the commonly used reductive/oxidative pulse polarity. For square wave depositions into sulfuric acid grown pores, the reductive/oxidative pulse polarity produces more uniform pore-filling, likely as a result of enhanced resonant tunneling through the barrier layer and reoxidation of copper in faster filling pores.     

Solution Layer Deposition: A Technique for the Growth of Ultra‐Pure Manganese Oxides on Silica at Room Temperature

With the ever increasing miniaturization in microelectronic devices, new deposition techniques are required to form high‐purity metal oxide layers. Herein, we report a liquid route to specifically produce thin and conformal amorphous manganese oxide layers on silicon substrate, which can be transformed into a manganese silicate layer. The undesired insertion of carbon into the functional layers is avoided through a solution metal–organic chemistry approach named Solution Layer Deposition (SLD). The growth of a pure manganese oxide film by SLD takes place through the decoordination of ligands from a metal–organic complex in mild conditions, and coordination of the resulting metal atoms on a silica surface. The mechanism of this chemical liquid route has been elucidated by solid‐state ²⁹Si MAS NMR, XPS, SIMS, and HRTEM.     

多孔氧化物块体材料的制备及其对重金属离子吸附研究进展

目前去除重金属离子的方法较多,其中吸附法因操作简单、经济性好而被广泛使用。多孔氧化物块体材料作为新兴的吸附材料具有比表面积高、机械强度高及可回收性好等特点,但吸附选择性差以及孔结构单一的缺陷限制了其在水体重金属处理中的应用。本文详细叙述了多孔氧化物块体材料的多种制备方法,并分别讨论了各方法的优势及其不足。介绍了近几年研究较多的多孔氧化物块体材料及其制备方法与特性。最后,对多孔氧化物块体材料对Pb、Cd及Cr等重金属离子吸附性能的影响因素及改善措施方面进行了总结分析,并指出多种材料的复合、材料表面的接枝改性及分级多孔结构的构建会增强对重金属离子的吸附性能。期望本文为多孔氧化物块体材料的制备及其在重金属离子吸附方面的应用提供参考。