水滑石负载的钯纳米粒子对水合肼的电催化氧化

利用共沉淀方法制备了载体水滑石(LDH), 通过离子交换法将PdCl2₄^- 插入水滑石层间, 再用水合肼将其还原, 制备得到了水滑石负载的分散状钯纳米粒子(LDH-Pd⁰). 利用X射线衍射(XRD)、透射电镜(TEM)和X射线电子能谱(XPS)等手段对所得样品进行了表征, 结果表明钯纳米粒子能很好地分散在水滑石上. 将该纳米材料修饰的玻碳电极(GCE)用于水合肼的电催化氧化, 该修饰电极表现出很好的电化学催化活性. 用循环伏安法(CV)、计时库仑法(CC)和计时安培法(i-t)对修饰电极的催化活性、有效表面积和水合肼的催化氧化机理等进行了研究. 结果表明水合肼在-0.1 V附近有明显的氧化峰, 在1.0×10^-5-2.0×10^-4 mol·L^-1范围内, 阳极峰电流与水合肼浓度间有良好的线性关系, 其检测限为9.5×10^-7 mol·L^-1. 计算得到GCE, LDH-Pd⁰/GCE 和LDH/GCE电极活化面积分别为0.02089, 0.02762 和0.02496 cm². 推知水合肼的氧化过程有4 电子和4 质子参与, 并且其在电极上的反应是受扩散控制的不可逆过程.     

铋在玻碳电极上电化学结晶初步研究(英文)

应用循环伏安法和计时安培法研究了铋在玻碳电极上的电结晶行为.循环伏安曲线显示了铋在玻碳电极上成核的典型特征,并表明其于玻碳电极上的电结晶是一个扩散控制过程.根据计时安培法响应曲线分析阐明了铋的浓度和过电势对成核生长机理的影响.进一步的定量测试表明该成核速率常数A和活化点密度N0随过电势增加呈现指数增大规律;扩散系数D随过电势增加呈指数衰减.以上实验结果至今未见报道.同时表明:Scharifker公式和Heerman公式均可用于本实验的理论解释.     

玻碳电极表面因瓦合金的电化学成核机理

在弱酸性因瓦合金(含镍质量分数为32~36 % 的镍铁合金)镀液中, 以线性扫描伏安法、循环伏安法和恒电位阶跃法对因瓦合金在玻碳电极表面的电沉积过程及其成核机理进行研究. 结果表明, 在该体系下, 因瓦合金在玻碳电极表面的电结晶属于扩散控制下的不可逆电极过程. 运用Scharifker-Hills理论模型(SH)拟合实验数据表明, 因瓦合金在玻碳电极表面的共沉积更加符合三维瞬时成核的成核规律. 运用Heerman-Tarallo理论模型(HT)分析得到因瓦合金在玻碳电极表面的成核生长的动力学参数, 当阶跃电位从-1.11 V变化至-1.17 V (vs SCE), 成核密度数(N₀)由0.72×10⁵ cm^-2提高至1.91×10⁵ cm^-2, 成核速率常数(A)从 40.35 s^-1增至 194.38 s^-1, 扩散系数(D)为(7.67±0.15)×10^-5 cm²•s^-1, 变化不大.     

电化学阶边精饰法制备钯镍合金纳米线的研究

运用连续恒电势三脉冲的电化学阶边精饰法在高定向石墨(HOPG)上制备钯镍合金纳米线阵列， 并研究了合金成分的影响因素. 结果表明，改变镀液组成可以调整钯镍合金成分，调整生长时间和生长电势来控制钯镍合金纳米线的直径. 用7 mmol•L^-1 PdCl2,3 mmo•L^-1 NiSO₄, 0.2 mol•L^-1 NH₄Cl，pH 8.5的混合溶液，控制脉冲电势-2.0 V形核0.2 s，在脉冲电势－0.4 V生长1 h，可以获得平均直径为200 nm, 长度约400 μm的钯镍合金纳米线阵列, 纳米线的合金成分中镍含量为12.4%(质量分数,w).     

侧链型磺化聚芳醚酮/磺化聚乙烯醇复合型直接甲醇燃料电池用质子交换膜

通过溶液共混法制备了不同磺化聚乙烯醇(SPVA)含量的侧链型磺化聚芳醚酮/磺化聚乙烯醇(S-SPAEK/SPVA)复合膜. 应用红外光谱(FTIR)对复合膜进行了表征, 扫描电镜(SEM)显示SPVA均匀分布在复合膜中. 通过对复合膜的性能测试发现该系列复合膜具有良好的热性能、较高的吸水率和保水能力. SPVA中的羟基能有效地阻碍甲醇的透过, 甲醇渗透系数从S-SPAEK/SPVA5 复合膜的7.9×10^-7 cm²·s^-1降低到S-SPAEK/SPVA30的1.3×10^-7 cm²·s^-1, 比S-SPAEK膜的11.5×10^-7 cm²·s^-1降低了一个数量级. SPVA的引入增加了亲水基团数量, 增加了复合膜的吸水和保水能力, 有利于质子按照“Vehicle”机理和“Grotthuss”机理进行传递, 柔软的SPVA链段与S-SPAEK侧链聚集成亲水相区, 形成连续的质子传输通道, 提高了复合膜的质子传导率. 在25 和80℃ 时, S-SPAEK/SPVA30 复合膜的质子传导率分别达到了0.071 和0.095 S·cm^-1. 可见,S-SPAEK/SPVA复合膜有望在直接甲醇燃料电池中得到应用.     

钒(Ⅳ/Ⅴ)电对在碳纸电极上的反应机理研究

采用循环伏安、极化曲线和交流阻抗技术研究了在0.8 mol·L^-1 VOSO₄+3.0 mol·L^-1 H₂SO₄中,V(Ⅳ/Ⅴ)电对在碳纸电极上的反应机理及可能的速度控制步骤。研究结果表明：V(Ⅳ/Ⅴ)电对在碳纸电极上的反应属准可逆过程,且氧化过程包含有后置化学转化步骤,计算得到VO²⁺的扩散系数为4.5×10^-5 cm²·s相似文献   

吲哚方酸菁半导体在场效应晶体管中的应用

研究了2,3,3-三甲基-1-H-吲哚方酸菁的场效应性质, 通过X射线衍射证实了方酸菁分子内电荷分离结构以及分子间面面堆积模式, 并在Si/SiO₂基片上通过真空蒸镀和旋涂的方法制备了p型晶体管器件. 通过对器件性能与沟道形态的研究, 我们发现退火处理能促进方酸菁薄膜由无定形态向多晶态转变, 从而使薄膜晶体管的迁移率从10^-5 cm²?V^-1?s^-1量级提高到10^-3 cm²?V^-1?s^-1量级. 顶接触结构单晶器件获得了7.8×10^-2 cm²?V^-1?s^-1的迁移率. 未封装的方酸菁晶体管在大气中也表现出较好的稳定性.     

10,10’-二甲基-3,3’-二磺酸基-9,9’-双吖啶的电致化学发光行为

研究了新试剂10,10'-二甲基-3,3'-二磺酸基-9,9'-双吖啶(简称DMDSBA)的电致化学发光(ECL)行为. 考察了电化学参数、反应介质以及pH等条件对DMDSBA电致化学发光信号的影响. 结果表明, 在玻碳电极上施加适当电压时, DMDSBA在KNO₃溶液介质中产生很强的电化学发光信号, 于优化的实验条件下, 发光强度的自然对数与DMDSBA浓度的自然对数在1.0×10^-5-1.0×10^-8 mol·L^-1范围内呈良好的线性关系,检出限可达2.3×10^-9 mol·L^-1. 并用循环伏安法、电致化学发光光谱以及荧光光谱, 研究了DMDSBA的电致化学发光机理.     

聚羟基丁酸-戊酸的非等温热分解反应动力学

用非等温TG-DTA技术, 在5.0、10.0、15.0和20.0 K•min^-1线性升温条件下, 研究聚羟基丁酸-戊酸(PHBV)的热分解反应动力学. 结果表明, 分解过程分三个阶段：分解初期、分解中期和分解后期. 分解初期的机理函数为Avrami-Erofeev方程(n=1/2), 对应随机成核和随后生长机理, 表观活化能E_a(β→0)为69.44 kJ•mol^-1, 指前因子A(β→0)为106.27 s^-1；分解中期的机理函数为Avrami-Erofeev方程(n =2/5), 对应随机成核和随后生长机理, 表观活化能Ea(β→0)为117.64 kJ•mol^-1, 指前因子A(β→0)为10^11.48 s^-1；分解后期的机理函数为Mampel Power法则(n=1/3), 对应机理为幂函数法则, 表观活化能Ea(β→0)为116.64 kJ•mol^-1, 指前因子A(β→0)为10^8.68 s^-1.     

脉冲辐解研究喹啉和异喹啉与瞬态粒子的反应

通过合理控制反应条件, 使体系在电子束脉冲作用后只剩下所需要的一种瞬态粒子, 用脉冲辐解研究了喹啉、异喹啉分别与水合电子、羟基自由基、氢自由基等几种典型的氧化还原瞬态粒子的反应过程, 研究了各种瞬态产物的吸收光谱及其变化规律, 测定了相关反应的速率常数. 喹啉、异喹啉与水合电子的反应速率常数分别为7.1×10⁹和3.4×10⁹ mol^-1·L·s^-1, 与羟基自由基的反应速率常数分别为7.2×10⁹和3.4×10⁹ mol^-1·L·s^-1, 与氢自由基的反应速率常数分别为5.7×10⁹和3.6×10⁹ mol^-1·L·s^-1. 这一结果表明, 喹啉、异喹啉均能够非常迅速地与水合电子、羟基自由基、氢自由基发生反应, 喹啉比异喹啉的反应速率更快. 运用电子理论分析了瞬态反应产物结构的稳定性差异, 结果表明, 喹啉的反应产物比异喹啉的稳定, 从而揭示了喹啉比异喹啉反应速率快的原因.     

Time Dependence of Current during Potentiostatic Growth of Clusters in Diffusion Mode of Electrodeposition

The fundamentally new model describes the initial current transients during the growth of clusters in the diffusion mode after instantaneous nucleation. The specific feature of the model is that it is based on the initial hemispherical diffusion of ions from bulk solution to the surface of growing clusters rather than on the period of Cottrell current decay. The subsequent overlapping of diffusion zones is taken into account by multiplying the current by a factor smaller than unity. The factor is equal to the ratio of true diffusion volume to the “extended” volume, which is equal to the overall volume of all diffusion hemispheres ignoring their overlapping. The results calculated by the model appeared to be rather close to those obtained using the conventional Scharifker–Hills–Mostany model, and, thus, confirm the correctness of this model. In this connection, the reasons for its inconsistency with the experimental data on the number of growing clusters remain unclear.     

电沉积二氧化锰成核机理及其充放电性能

采用计时电流法沉积纳米MnO₂电极材料,利用Scharifker-Hills成核理论模型分析时间-电流(i-t)曲线判断了MnO₂成核机理。 对3种不同的成核方式制得的MnO₂材料进行电化学超级电容性能测试、用SEM观察了其微观形貌。 比较了不同沉积方法对沉积材料结构、电容性能的影响。 计时电流测试发现,在0.1 mol/L Mn²⁺溶液中,电势阶跃至0.365 V,初始成核符合瞬时成核机理,在0.01 mol/L Mn²⁺溶液中,电势阶跃至0.418 V,初始成核存在瞬时成核和连续成核两种不同机理,在0.5 mmol/L Mn²⁺溶液中,电势阶跃至0.515 V,初始成核则符合连续成核机理。 超级电容性能测试发现,瞬时成核下制得的MnO₂电极材料相对于另外两种成核方式得到的电极材料具有更好的电容性能,这是因为瞬时成核更易于形成多孔、纳米片(棒)状等高比表面积的沉积物,表明制备方法影响MnO₂电极材料电容性能。     

从2AlCl3/Et3NHCl离子液体中电沉积制备Ni 和Ni-Al 合金

在含Ni2+的2AlCl3/Et3NHCl离子液体中的铜电极上通过恒电位电沉积制备出金属Ni和Ni-Al合金.采用循环伏安和计时电流方法,揭示铜电极上沉积金属Ni的成核机理,研究了电沉积Ni-Al合金的机理,以及恒电位沉积Ni-Al合金工艺条件对沉积Ni-Al合金表面形貌和电流效率的影响.结果表明:在铜电极上电沉积金属Ni的成核机理为受扩散控制的三维瞬时成核过程.在电量≥3.0 C时,电沉积Ni-Al合金的组成基本不再变化.Ni-Al合金的电沉积机理为,Ni的电沉积受扩散控制,同时进行Al的欠电位沉积,在Ni-Al合金电沉积过程中某些Ni-Al合金相的沉积可能受动力学限制而使Ni-Al合金的组成偏离热力学预测结果.在电沉积Ni-Al合金的沉积电流小且平稳,电沉积速率慢条件下,Ni-Al合金表面形貌致密均一,反之就会出现瘤节.电沉积Ni-Al合金的电流效率＞90％.电沉积物的组成接近于Ni3Al合金.     

Pt-Ni与Pd-Ni纳米薄膜的电化学制备和乙醇电催化性能研究(英文)

通过电沉积法在Ti基体上制备具有纳米结构的Pt-Ni和Pd-Ni薄膜,前者呈纳米花瓣形状,厚度为10～20 nm,后者主要由纳米颗粒组成,大小为50～60 nm.XRD测试结果显示,Pt-Ni和Pd-Ni纳米薄膜结晶程度较差.循环伏安法测试薄膜对乙醇电催化氧化的性能,结果表明Pt-Ni和Pd-Ni纳米薄膜可使乙醇起始氧化电位分别负移至-0.74 V和-0.71 V,且在碱性介质中加Ni可提高催化剂的活性和抗毒化性能.     

碱性介质中多孔纳米结构镍/钯-镍电极上甲醇电氧化反应(英文)

A nanostructured Ni/Pd-Ni catalyst with high activity for methanol oxidation in alkaline solution was prepared by electrodeposition followed by galvanic replacement, that is, electrodeposition of Ni-Zn on a Ni coating with subsequent replacement of the Zn by Pd at the open circuit potential in a Pd-containing alkaline solution. The surface morphology and composition of the coatings were examined by energy dispersive X-ray spectroscopy and scanning electron microscopy. The Ni/Pd-Ni coatings were porous and were composed of discrete Pd nanoparticles of about 58 nm. The electrocatalytic activity of the Ni/Pd-Ni electrodes for the oxidation of methanol was examined by cyclic voltammetry and electrochemical impedance spectroscopy. The onset potentials for methanol oxidation on Ni/Pd-Ni were 0.077 V and 0.884 V, which were lower than those for flat Pd and smooth Ni electrodes, respectively. The anodic peak current densities of these electrodes were 4.33 and 8.34 times higher than those of flat Pd (58.4 mA/cm2 vs 13.47 mA/cm2) and smooth Ni (58.4 mA/cm2 vs 7 mA/cm2). The nanostructured Ni/Pd-Ni electrode is a promising catalyst for methanol oxidation in alkaline media for fuel cell application.     

Electrochemical deposition of indium: nucleation mode and diffusional limitation

the electrochemical deposition of indium metal from InCl₃ solutions was investigated. Cyclovoltammetric experiments showed that the initial hydrogen evolution reaction, observed together with the metal deposition on Pt surface, is blocked when the surface is covered by In. At large cathodic potentials, the current is diffusion-limited. The scan rate dependence of cyclovoltammograms allowed the determination of the diffusion coefficient of In³⁺ ions, 8.18 × 10^–6 cm²/s, using the Delahay equation. The activation energy of diffusion, determined from the temperature dependence of cyclovoltammograms, is about 0.3 eV (23 kJ/mol). Chrono-amperometric experiments are consistent with the cyclovoltammetry; the In³⁺ diffusion coefficient determined using the Cottrell law is in good agreement with the value determined by the Randles-?ev?ik equation. Moreover the use of the nucleation models developed by Scharifker and Hills showed a progressive nucleation mode. Electron microscopy observations and X-ray diffraction patterns confirmed the formation of crystalline indium deposits.     

Study of hydrogen electrosorption in Pd-Ni alloys by the quartz crystal microbalance

The electrochemical quartz crystal microbalance (EQCMB) method has been used to study the processes of hydrogen absorption/desorption in Pd-Ni alloy electrodes. It was found that hydrogen electrosorption is accompanied by an additional frequency shift, attributed to the stresses generated inside the alloy. The influence of stresses on the EQCMB response depends on the amount of absorbed hydrogen and the alloy composition. From the comparison of the EQCMB results with Pd-Ni alloy absorption capabilities data, it was concluded that the decrease of the hydrogen sorption capacity at a Ni content of ca. 25–30 at% is due to an excessive generation of stresses in the alloy lattice. Also, a dependency of the rate of hydrogen absorption in Pd-Ni alloys on potential is reported. Electronic Publication     

Effect of H<Subscript>2</Subscript>SeO<Subscript>3</Subscript> on the early stages of nucleation and growth during Cu electrocrystallization in acidic medium on glassy carbon electrode

The early stages of Cu electrodeposition onto a GC electrode were investigated in 0.5 M H₂SO₄ + 0.01 M CuSO₄ solution without or with H₂SeO₃ when a molar concentration ratio [Cu(II)]/[Se(IV)] was 1.10⁴ to 2.10². The H₂SeO₃ solution in 0.5 M H₂SO₄ was also used. The electrochemical techniques such as cyclic voltammetry and chronoamperometry and structural investigation using ex situ AFM were applied to study the nucleation and growth of Cu onto a GC electrode. Chronoamperometric results were shown to follow an instantaneous 3D nucleation and diffusion-controlled growth model by Scharifker and Hills. The values of number of Cu nuclei N and average nuclei radius r _av were calculated. It was shown that, in the presence of H₂SeO₃ in amounts of 0.001 to 0.005 mM, N increases and r _av decreases. At higher concentrations of the additive, the changes of these parameters with the deposition potential E _dep were shown to be somewhat more complex. The dependences of N and r _av on the concentration of H₂SeO₃ in different regions of Cu overpotentials were also revealed.     

Scanning electrochemical microscopy and video microscopy investigations of Tiron-mediated polypyrrole nucleation on AA2024-T3

Scanning electrochemical microscopy (SECM) and video microscopy have been used to examine the mediated electrodeposition of polypyrrole on AA2024-T3. Of particular interest is the role of surface heterogeneity (namely, copper-rich secondary phase particles) on electrodeposition mediated by 4,5-dihydroxy-1,3-benzenedisulfonic acid (Tiron). SECM shows that polymer nucleation occurs exclusively on the aluminum matrix of the alloy. Video microscopy shows this to be true on a model alloy (a pure Al substrate with an embedded Cu wire) as well, and also suggests that polymer growth is directional toward the copper-rich sites in the absence of sulfate in the deposition solution. A model is presented in which polymer deposition on the copper-rich sites is inhibited either by CuSO₄-induced passivation or by the loss of mediator due to Cu–Tiron complex formation.