氯霉素分子印迹聚合膜电极的制备及氯霉素检测

以邻氨基酚(OAP)为功能单体,氯霉素(CAP)为模板分子,用电化学聚合的方法在Pt上合成了CAP分子印迹（MIP）OAP膜(CAP-MIP-OAP/Pt)电极,通过扫描电子显微镜和电化学技术对聚合膜的结构和性能进行了表征。 结果表明,该膜电极对CAP检测有较好的选择性和灵敏度,CAP检测的线性范围为4.33×10-8～3.09×10-6 mol/L,检出限为2.5×10-8 mol/L。     

聚(苯胺-co-邻氨基酚)修饰玻碳电极的制备及其对抗坏血酸的电化学氧化

研究了苯胺(AN)与邻氨基酚(OAP)在玻碳电极表面的电化学共聚,由此制备了AN与OAP共聚物膜修饰的玻碳电极(PAN-OAP/GCE/CME),并研究了该电极的电化学行为及其对抗坏血酸(AA)的电催化氧化。研究表明:AN与OAP的共聚速率随溶液中OAP浓度的增大而减小。当OAP与AN的浓度比>1∶10时,聚合行为相似;在其浓度比为1∶10时得到的共聚膜具有较好的电化学活性。由此可在0.1mol/L磷酸缓冲溶液(PBS,pH6.8)中对AA进行电催化氧化。在PAN-OAP/GCE/CME上其氧化峰电位位于0.21V,比在裸玻碳电极上(0.53V)降低了0.32V。该共聚物膜在中性溶液中显示出较好的电化学活性,为生物样本中AA的测定提供了条件。AA在修饰电极上的响应电流与其浓度在0.05~16.5mmol/L范围内呈线性关系,r=0.9998。采用计时电流法对AA催化氧化的扩散系数和催化速率常数进行了研究。     

邻氨基酚在硫堇分子自组装膜修饰金电极上的电化学行为及其测定

在 0 .0 5 mol/L p H4.2的 HAc- Na Ac- PHP(邻苯二甲酸氢钾 )缓冲溶液中 ,用硫堇分子自组装膜修饰金电极对邻氨基酚的电化学行为进行了初步研究。研究发现 ,邻氨基酚在 - 0 .1 V左右出现一可逆氧化还原峰 ,在 0 .38V( vs.SCE)左右产生一阳极峰。两峰均由邻氨基酚的氧化还原引起 ,较正处的阳极峰表现出吸附波的性质 ,该峰较灵敏 ,适于伏安测定。该峰的峰电流与邻氨基酚的浓度在 1 .0× 1 0 - 6 ～ 5 .0× 1 0 - 4mol/L范围内呈线性关系 (相关系数 r =0 .9991 )。该方法可用于邻氨基酚含量的测定     

碳柱热电极的制备及应用

用铅笔芯制作了不同直径的碳柱热电极,表征了碳柱热电极的电化学和温敏等各种性质。结果表明,碳柱热电极在多次加热过程中均表现出对温度变化的快速响应以及良好的热稳定性。将其应用于痕量铅的方波阳极溶出伏安法测定,65℃时灵敏度比常温高,Pb2＋浓度在1~22μg/L呈线性关系,线性回归系数r=0.995 5,检测限0.5μg/L。     

硫酸溶液中Pt(111)电极面上存在SO2-4的XPS证据

Pt（111）电极在硫酸溶液中的循环伏安图已被多个研究小组所得到[1-3]．对图上出现的高于正常氢吸脱附电位出现的两个电流峰（Clavilier等[1]首次发现并称之为异常峰）的解释至今没有得到一致意见．分歧焦点是异常峰的出现是由于强键合吸附氢还是吸附其它阴离子所致·本文用XPS和LEED研究异常峰电位处浮出的Pt（111）电极表面，发现尖锐异常峰的出现是由于表面上吸附了离子．1实验文献＊中详细说明了实验所用装置．主要部份是把装有XPS、LEED、MS、Ar“枪的超高真空腔门HV）与测量循环伏安图的腔（EC）联在一起·UHV中基压强为4x…     

基于探究式教学模式对预阳极化前后的玻碳电极测定对乙酰氨基酚的伏安图差异的分析及机理讨论

基于电极反应活化能,预阳极化前后玻碳电极表面结构变化及氢键催化作用,以探究式教学模式讨论了预阳极化前后的玻碳电极测定对乙酰氨基酚的伏安图差异形成的原因。这种教学模式不仅有利于提高实验课教学质量,也会促进教师自身业务能力的提高。     

对羟基苯甲酸分子印迹传感器的制备及其性能研究

采用简单高效的分子印迹膜技术,制备了对羟基苯甲酸(PHA)分子印迹传感器。敏感膜采用循环伏安法(CV)在玻碳电极表面合成,采用CV、微分脉冲伏安法、线性扫描伏安法和电化学交流阻抗法在K3[Fe(CN)6]/K4[Fe(CN)6]溶液中测试此分子印迹传感器的性能。在最优条件下,PHA检测线性范围为0.6～8.0μmol/L,检测限(S/N=3)为0.2μmol/L。实验结果表明:该分子印迹传感器灵敏度高、选择性好并且具有良好的再生性能,传感器对与PHA结构相似的分子有较强的抗干扰能力,可望用于植物体分泌化感物质PHA的实时监测。     

溶剂聚合膜pH电极作内电极的气敏电极的研究

研究了以中性载体为活性物的石墨内导平头溶剂聚合膜(SPM)pH电极作内电极的二氧化碳和氨气敏电极。电极的性能取决于中性载体的特性,其中以菸酸十八酯为内电极膜活性物的二氧化碳气敏电极和以二辛基十八胺为活性物的氨气敏电极性能较佳。二氧化碳气敏电极用作丙酮酸脱羧酶酶电极的原电极,其性能院于传统的以玻璃pH电极作内电极的二氧化碳气敏电极。     

铋(Ⅲ)-8-羟基喹哪啶体系极谱行为——表面活性剂增敏机理和分析应用——Ⅱ.铋(Ⅲ)-8-羟基喹哪啶络合物电极反应和十二烷基苯磺酸钠增敏机理

试验表明,铋(Ⅲ)-8-羟基喹哪啶(8-OXQ)络合物(pHll,-0.60V)的峰电流(p)具吸附特性,为准可逆电极反应过程,其电子转移数(n),传递系数(α)及饱和吸附量(Γ_ο)分别为3,0.45,6.5×10~(-12) mol/cm~2。加入十二烷基苯磺酸钠(SDBS)未形成三元络合物,因SDBS的超载强烈吸附,引起诱导吸附,电双层结构激烈变化,而使电流峰形巨变,电流峰高(i_p)增大10余倍。讨论并指出SDBS对Bi(Ⅲ)与8-羟基喹啉(8-OX)及衍生物络合吸附电流增敏或抑制,与试剂组分、结构、解离态及络合物存在状态、电荷数、符号有关。     

Effect of Some Metal Ion Dopants on Electrochemical Properties of Ni （OH）2 Film Electrode

The Ni(OH)2 film electrodes doped respectively with alkali-earth metals aluminum, lead, partial transi-tion metal and some rare-earth metal (altogether 17 kinds of metals) ions were prepared by cathode electrode-position. The electrode reaction reversibility, the difficult extent of oxygen evolution, the proton diffusion coefficient, the discharge potential of middle value and the active material utilization of the Ni(OH)2 film elec-trode were compared with those of the ones doped with the metal ions by means of cyclic voltammetry, poten-tial step and constant current charge-discharge experiments. It was found that Ca^2 , Co^2 , Cd^2 , Al^3 etc. have obviously nositive effect.     

Studies on Some Nickel(II) and Cobalt(II) Mixed Ligand Complexes of Arylsalicyl-Aldimine and Other Ligands

Several new mixed ligand complexes of Ni(II) and Co(II) of p-tolylsalicylaldimine (Sal-TH) or p-anisylsalicylaldimine (Sal-AH) with 8-hydroxyquinoline (HOx), benzohydroxamic acid (BH₂) or α-picoline (α-pic) have been synthesized. The complexes have the general formulae: [M(Sal-T)L],[M(Sal-A)L]⋅H₂O or [Ni(Sal-T)₂(α-pic)₂]⋅H₂O where M=Ni(II) or Co(II), Sal-T=p-tolylsalicylaldiminate, Sal-A=p-anisylsalicylaldiminate, L=8-hydroxyquinolinate or benzohydroxamate and α-pic=α-picoline. Analytical, conductivity and spectral data support a square planar structure for Co(II) complexes and octahedral structure for Ni(II) complexes. The thermal behaviour of the complexes has been studied by TG and DTG techniques. It was proposed that the decomposition of the complexed Schiff base takes place via a radical mechanism while for 8-hydroxyquinolinate or benzohydroxamate via proton transfer. Kinetic parameters of the thermal decomposition process have been computed by means of Coats-Redfern and Horowitz-Metzger methods. This revised version was published online in August 2006 with corrections to the Cover Date.     

酞菁镍-表面活性剂薄膜修饰电极及其催化性能的研究

将酞菁镍(NiPc)掺入阳离子表面活性剂双十二烷基二甲基溴化铵(DDAB)的氯仿溶液中,并涂布于热解石墨电极表面,待氯仿挥发后制得NiPc-DDAB薄膜电极。循环伏安实验表明,在KBr溶液中,该薄膜电极有两对良好且稳定的还原氧化峰,第一对峰的E_pc1=-0.64V,E_pa1=-0.60V(vs.SCE);第二对峰的E_pc2=-0.84V,E_pa2=-0.80V,本文着重探讨了第二对峰的电化学行为,估计了该体系的电化学参数如电子扩散系数De和非均相电极反应速率常数k^0'.该薄膜电极可用于催化各种卤代乙酸的电化学还原,用多种表面分析技术对该薄膜进行了表征。     

掺杂多壁碳纳米管改性聚溴甲酚绿膜修饰电极的制备、表征与应用研究

研究了掺杂多壁碳纳米管(MWNT)改性聚溴甲酚绿膜(PBG),以不同修饰方法制备了4种修饰电极,用扫描电镜、交流阻抗及循环伏安法等对电极进行表征。结果表明:4种修饰电极的电活化面积均得到明显提高,其中以层层修饰制备的聚溴甲酚绿膜/多壁碳纳米管复合膜(PBG/MWNT/GC)电极最能发挥MWNT和PBG的电活性。将电极用于8-羟基喹啉(8-HQ)电化学行为的研究,结果表明:4种修饰电极的伏安响应明显提高,且8-HQ在PBG/MWNT/GC上的氧化峰电位负移最多,峰电流最大,约为裸玻碳电极的4.5倍,电催化作用显著增强。8-HQ在PBG/MWNT/GC上电极反应的电子转移数和质子数均为1,是吸附控制的不可逆电氧化过程,氧化峰电流Ip与浓度c在4.0×10-6～3.5×10-4mol/L范围内呈良好的线性关系,r=-0.997 2,检出限(S/N=3)为1.96×10-8mol/L。PBG/MWNT/GC修饰电极可实现8-HQ的快捷、简便测定。     

Electrochemical Behaviour of Magnesium(II) on Ni Electrode inLiCl-KCl Eutectic

The electrochemical behaviour of magnesium(II) and the formation mechanism of Mg-Ni alloys on Ni electrode were studied in LiCl-KCl eutectic using various electrochemical techniques. Cyclic voltammogram and square-wave voltammogram revealed that under-potential deposition of magnesium occurred on Ni electrode because Mg-Ni alloy compounds were formed. The thermodynamic properties of the Mg-Ni intermetallics, Mg₂Ni and MgNi₂, were determined using open circuit chronopotentiometry in the temperature range of 818―893 K. Moreover, the Mg-Ni alloys were produced by potentiostatic and galvanostatic electrolysis under different conditions and characterized by means of scanning electron microscopy(SEM) equipped with energy dispersive spectrometry(EDS) and X-ray diffraction(XRD). The experimental results indicate that Mg-Ni intermetallic compounds can be selectively produced by potentiostatic electrolysis.     

Silver-Selective Electrode Based on a Direct Modified Electrode Silver Hexacyanoferrate(II) Film

ABSTRACT

A silver hexacyanoferrate(II) modified electrode is introduced as a silver-selective electrode. The electrode was prepared based on a new type of chemically modified electrodes by direct modification of the electrode surface. The electrode response characteristics were investigated by potentiometry. The calibration curve of the electrode shows a linear potentiometric response to Ag⁺ in the range of 10^-7 - 10^-2 M with detection limit of 5 × 10^-8. The modified electrode described in this paper is very simple, low cost and has linear response to Ag⁺ with a slope of 52-55 mV per decade.     

Voltammetric Detection of the Herbicide Metamitron at a Bismuth Film Electrode in Nondeaerated Solution

In this work, we present a novel application of bismuth film electrodes (BiFE) for the direct analysis of the herbicide metamitron (4‐amino‐3‐methyl‐6‐phenyl‐1,2,4‐triazin‐5one) in nondeaerated solutions by square‐wave voltammetry (SWV) and differential pulse amperometry. Bismuth films were plated ex‐situ onto carbon paste electrodes (CPE) by 240 s deposition at ?0.600 V from a 0.10 M acetate buffer (pH 4.5) containing 0.50 mM bismuth nitrate. Metamitron SWV analytical signals were registered in 0.10 M acetate buffer (pH 4.5) solutions, where the herbicide reduction takes place at ?0.675 V. The metamitron signals obtained with BiFE have the double sensitivity and a 50 mV positive potential shift when compared to those obtained with plain CPE. Under these conditions, the dynamic linear range of concentrations is comprised between 10 and 200 μM and the detection limit is 2 μM.     

普鲁士蓝膜修饰电极的电化学阻抗谱

测量了应用电化学方法制备的不同厚度的普鲁士蓝膜修饰电极的循环伏安行为与电化学阻抗谱.由所得到的循环伏安图讨论了普鲁士蓝修饰膜的氧化还原过程,并对相关的Nyquist图进行了解析,提出了相应的等效电路.在此基础上计算出较薄膜中普鲁士蓝/普鲁士白电化学反应的表观速率常数和表观扩散系数,讨论了膜厚度对电荷扩散的影响.当膜相对较薄时,电极过程主要由动力学过程控制;当膜达到一定厚度时,电荷在膜中的扩散速率受到限制,电极过程由动力学过程和电荷扩散过程共同控制,证实了文献报导的普鲁士蓝膜修饰电极为多层空间分布电荷传递模型.     

Investigation of Copper(II) Interference on the Anodic Stripping Voltammetry of Lead(II) and Cadmium(II) at Bismuth Film Electrode

The bismuth‐coated electrode is known to be prone to errors caused by copper(II). This study investigates copper(II) interference at bismuth film electrode for the detection of lead(II) and cadmium(II). It was conducted using glassy carbon electrode, while the bismuth film was plated in situ simultaneously with the target metal ions at ? 1200 mV. Copper(II) presented in solution significantly reduced the sensitivity of the electrode, for example there was an approximately 70 % and 90 % decrease in peak signals for lead(II) and cadmium(II), respectively, at a 10‐fold molar excess of copper(II). The decrease in sensitivity was ascribed to the competition between copper and bismuth or the metal ions for surface active sites. Scanning electron microscopy (SEM) and energy dispersive X‐ray (EDX) analysis suggested a large decrease in the amount of bismuth nanoparticles formed on the electrode surface in the presence of copper(II) occurred, validating the competition between copper and bismuth ions for surface active sites. Recovery of the stripping signal of lead(II) and cadmium(II) was obtained by adding ferrocyanide ion to the solution. Finally, the proposed method was successfully applied to determine lead(II) and cadmium(II) in water samples and the method was validated by ICP‐MS technique.     

八-羟基喹啉铝薄膜光致发光的厚度依赖性质

In situ thickness dependent photoluminescence (PL) measurements of tris(8-hydroxyquinoline) aluminum(Alq3) film were performed. At the beginning of Alq3 deposition on the glass substrate, the Alq3 emission showed a sharp red-shift. Further deposition of Alq3 resulted slight red-shift, and finally tended to saturated value. The total red-shift of about 12 nm was observed for the Alq3 film thickness range from 2 to 500 nm.This red-shift was attributed to the change from the 2D to 3D exciton state with increasing Alq3 film thickness. Meanwhile, the PL intensity of Alq3 emission increased continuously, and showed a rate change at the initial deposition of Alq3 due to non-rediative decay of excitons arised from the interaction between excitons and the substrate, and finally tended to saturation with the Alq3 thickness.