一维有序聚苯胺纳米阵列的制备及电化学储能性能

以导电玻璃FTO为基底电极, 在硫酸溶液中, 分别研究了苯胺单体浓度和恒定电流大小对聚苯胺(PANI)形貌的影响; 同时恒定苯胺单体的浓度和工作电流, 探究了不同类型的质子酸对PANI阵列形貌的影响. 结果表明, 采用恒电流方法可以制备出一维有序PANI纳米线阵列, 而且当苯胺的浓度为0.1 mol/L, 恒电流法的工作电流密度为0.03 mA/cm²时, 所制备的PANI纳米线阵列形貌最佳; 当用HCl, HNO₃和对甲苯磺酸(p-TSA)作为合成PANI的支持液时, 得到树桩状的PANI 纳米结构, 不能得到均一的纳米线阵列结构. 电化学性能测试结果表明, 制备的最佳形貌PANI纳米线阵列的比电容值可达560 F/g; 循环1000周后电容损失率为11%.     

ZnO-聚苯胺同轴纳米线及其列阵的制备和表征

以阳极氧化铝膜 (AAO)作模板 ,制备聚苯胺 (PANI)纳米管和PANI纳米管列阵 ;同时利用溶胶_凝胶法制备ZnO_PANI同轴纳米线和同轴纳米线列阵 .PANI纳米管和ZnO_PANI同轴纳米线的形貌通过透射电子显微镜表征 .PANI纳米管的外径约 3 0nm ,内径约 1 0nm ;ZnO_PANI同轴纳米线直径约 60nm .实验发现 ,较之ZnO纳米线 ,同轴AAO模板中纳米线列阵的可见光发射谱带兰移 ,强度显著增强 ,这可能和PANI链上的NH基团与表面Zn2 +离子之间的相互作用有关 ,以及由于ZnO纳米微粒在PANI上富集、PANI的光生载流子部分转移给ZnO微粒所致 .实验还发现分散在NaOH溶液中的同轴纳米线 ,其可见光发射谱带比AAO模板中同轴纳米线的谱带兰移更甚     

CdSe纳米线阵列的制备及其表征(英)

通过在含有SeSO₃^2-和Cd²⁺的室温水溶液中，用模板-电沉积法在纳米孔阵列阳极氧化铝膜(AAM)模板中制备了高有序性的CdSe纳米线阵列，并对其形貌、结构和组分进行了表征。扫描电子显微镜(SEM)和透射电子显微镜(TEM)结果表明，纳米线阵列中的CdSe纳米线具有相同的长度和直径，分别对应于使用的AAM模板的厚度和孔径；X-射线衍射(XRD)和X-射线能谱(EDAX)结果表明，CdSe纳米线中Cd和Se的化学组成非常接近于1∶1，其结构为立方CdSe。另外，对模板-电沉积法制备CdSe纳米线的机理进行了讨论。     

电致变色型导电聚苯胺固态超级电容器的构建与性能研究

以苯胺硫酸溶液为沉积液,导电玻璃(FTO)为基底材料,在-0.2~1.2 V范围内先电位扫描一圈生成聚苯胺(PANI)晶种,然后在-0.2~0.8 V范围内用循环伏安法电沉积导电PANI材料.所得样品用红外光谱和扫描电子显微镜进行结构表征;以最佳循环伏安电沉积条件制备的PANI/FTO为活性电极,以H_2SO_4/聚乙烯醇(H2SO4/PVA)为凝胶电解质组装了电化学电容器,通过循环伏安、恒电流充放电和电化学阻抗法研究了组装电化学电容器的电化学性能.研究结果表明,以H_2SO_4/PVA凝胶电解质,沉积于导电玻璃表面的PANI活性电极材料的面比电容可达172.7 m F/cm~2,并且在2000次充放电以后,比电容值仍可保留初始值的92.8%.以分区沉积有PANI的导电玻璃可组装制备通过变色显示充放电过程的电化学电容器,在充电时,其颜色逐渐从浅绿色向深绿色转变,放电时,颜色逐渐从深绿色向浅绿色转变.     

氧化剂对磺化石墨烯负载聚苯胺复合材料结构与电化学性能的影响

以磺化石墨烯(sGNS)为基板材料,通过界面聚合方法制备出不同分级结构磺化石墨烯负载聚苯胺(sGNS/PANI)复合材料,并系统研究了氧化剂类型对复合材料的化学组成、形貌结构和超级电容特性的影响.结果显示,过硫酸铵为氧化剂合成的复合材料中PANI的产率和氧化程度最高,其形貌呈现出sGNS垂直生长PANI纳米短棒阵列结构,PANI的共轭程度和结晶性均较高,从而赋予复合材料高的比电容(497.3 Fg-1),以及良好的倍率特性和循环稳定性(2000次循环后比电容仅损失5.7%).当以三氯化铁为氧化剂时,复合材料中PANI的得率很低,并在sGNS表面形成较薄的包覆层,此时复合材料的比电容最低(228.5 Fg-1),但充放电循环性能较好(2000次循环后比电容的保持率为87.4%).当氧化剂为高锰酸钾时,复合材料中PANI以团聚态颗粒无规堆积在sGNS表面,PANI以无定型结构存在,其比电容虽然较高(419.6 F g-1),但其倍率特性和充放电循环性能较差(2000次循环后比电容损失19.9%).     

双槽法电沉积Cu/Ni多层纳米线有序阵列

以多孔阳极氧化铝（AAO）为模板，采用双槽法电沉积工艺制得高度有序的Cu/Ni多层纳米线阵列。利用扫描电镜（SEM）和透射电镜（TEM）对Cu/Ni多层纳米线进行了表征，观察到纳米线表面平滑，多层结构清晰，各子层厚度均匀，直径约为 100 nm，与AAO模板孔径基本一致。由选区电子衍射（SAED）照片可知，多层纳米线中Cu层和Ni层均为单晶结构。振动样品磁强计（VSM）测试结果表明，Cu/Ni多层纳米线阵列具有明显的垂直磁各向异性，外加磁场垂直和平行于AAO模板表面时，磁滞回线的矩形比分别为 0.701 和 0.101 ，矫顽力分别为 589 Oe和 202 Oe。通过控制铝阳极氧化工艺及电沉积时间，可获得不同直径、不同子层厚度的Cu/Ni多层纳米线阵列。     

阳极氧化铝模板法可控制备金属纳米线和纳米管阵列的生长机制

利用阳极氧化铝模板(AAO)进行Ni的电化学沉积, 通过在溶液中引入螯合剂控制电解质的有效浓度和电沉积的过电位, 实现了Ni纳米线和纳米管阵列的可控制备. 通过分析电沉积过程中纳米线和纳米管在不同位置生长速率(侧壁(Vw)和底端(Vb))的控制因素, 我们提出了纳米线和纳米管生长的可能机制. 当电解质浓度高而还原电位更负(如-1.5 V)时, 或者当电解质浓度低而还原电位较负(如-0.5 V)时, Vw>Vb, 可以获得Ni纳米管阵列; 当电解质浓度高而还原电位较负(如-0.5 V)时, 或者当电解质浓度低而还原电位更负(如-1.5 V)时, Vw≈Vb, 可以获得Ni纳米线阵列. 这种生长机制适用于多种金属纳米管或者纳米线阵列的可控制备.     

Pt纳米线阵列的氧还原催化性能

采用阳极氧化铝(AAO)模板法电化学沉积制备了Pt纳米线阵列(Pt NWs)氧还原催化剂, 通过扫描电子显微镜(SEM)、透射电子显微镜(TEM)和电化学测试对Pt纳米线阵列催化剂的形貌和电催化性能进行了表征. 循环伏安法(CV)研究表明Pt纳米线阵列催化剂的电化学活性面积大于其几何面积; 旋转圆盘电极(RDE)测试研究发现, 制备的Pt纳米线阵列催化剂的氧还原反应(ORR)曲线的半波电势相对Pt/C的有正移, 并且Pt纳米线阵列催化剂的极限扩散电流比Pt/C大.     

石墨烯修饰Y型TiO_2纳米管光电极制备及其对氨氮催化氧化性能

采用三步阳极氧化法和一步循环伏安电沉积法制备了还原氧化石墨烯(rGO)修饰的Y型TiO_2纳米管(rGO/Y-TiO_2NTs)电极。通过场发射电子扫描显微镜(FESEM)、X射线能谱(EDS)、X射线衍射(XRD)、紫外可见漫反射光谱(UV-Vis DRS)及拉曼光谱(Raman)等对电极样品进行了表征。以rGO/Y-TiO_2NTs电极为光阳极,测试了不同循环伏安沉积圈数对电极光电流响应的影响,考察了在1.0 V偏压下电极对氨氮的光电催化氧化性能。结果表明,高度有序的Y-TiO_2NTs为锐钛矿型,具有大的比表面积,表面修饰平滑透明rGO薄膜后可显著提高其光电催化效率,沉积圈数为30时电极在30 min内对氨氮的光电催化氧化效率为95.9%。     

溶剂散逸自组装法制备具有电致收缩性能的聚苯胺/聚氨酯凹透镜阵列

以水珠为模板,采用溶剂散逸自组装法制备了表面具有特殊形貌的有序多孔膜. 以此多孔膜为模板制备了聚苯胺/聚氨酯（PANI/PU）的凹透镜阵列. 采用红外光谱（FTIR）和扫描电子显微镜（SEM）对界面聚合得到的PANI/PU纳米复合物的结构和凹透镜阵列的形貌进行了表征,研究了不同合成条件对纳米复合物导电性能的影响,并对PANI/PU凹透镜阵列的电学和光学性能进行了研究. 结果表明,PANI/PU凹透镜阵列同时具有导电性、电致收缩性和光衍射性质;其收缩率与外加电压成反比,而透光率与收缩率成正比.     

High-performance supercapacitor based on ultralight and elastic three-dimensional carbon foam/reduced graphene/polyaniline nanocomposites

A novel supercapacitor based on ultralight and elastic three-dimensional porous melamine foam-derived macroporous carbon/reduced graphene oxide/polyaniline nanocomposites were fabricated, which showed great electrical performance and cycle performance.     

聚苯胺-还原氧化石墨烯复合材料的比电容及超级电容性能

Flaky polyaniline-reduced graphene oxide (PANI-rGO) composites have larger specific capacitance due to the improved redox charge of PANI in the composites, fabricated by simultaneous reduction of PANI-GO. The structural and morphological analyses were carried out using scanning electron microscopy, UV-Vis spectroscopy, and thermogravimetry. The results showed that the composites are flaky in shape. PANI is uniformly coated on GO, and PANI-rGO has specific capacitance as high as 1069 F·g^-1 (1.71 F·cm^-2) at a current density of 20 A·g^-1, 5 times higher than PANI-GO; this is caused by the large surface and conductivity of the rGO in the composite.     

纳米纤维聚苯胺在电化学电容器中的应用

采用脉冲电流方法（PGM）合成了具有纳米纤维结构的导电聚苯胺（PANI）.扫描电子显微镜对膜层观察表明, PANI膜是由直径约为100 nm的掺杂态聚苯胺纤维交织而成.以纳米纤维状聚苯胺组成电化学电容器,研究了其电化学电容性能,并与恒电流方法（GM） 制备的颗粒状PANI电容器性能进行了比较.结果表明,在相同的沉积电量下,PGM制备的纳米纤维状PANI电化学电容器比颗粒状PANI电化学电容器具有更大的电容容量,其电化学电容器的比电容可高达699 F•g－1,能量密度为54.6 Wh•kg－1.并且该电化学电容器具有良好的充放电性能和循环寿命.     

自支撑三维功能化石墨烯/聚苯胺电极材料的制备及超级电容性能

采用水热法制备了三维石墨烯(3D-G),并以十八胺(ODA)为接枝剂对部分还原的氧化石墨烯进行氨基化处理,再利用原位聚合法在氨基化石墨烯表面生长聚苯胺,制备了十八胺功能化石墨烯/聚苯胺(G-ODA/PANI).对材料进行了结构表征、电化学性能分析和材料结构的比电容贡献分析.结果显示,电极材料的电容贡献大部分体现为材料的表面电容,G-ODA/PANI电极片在1 A/g电流密度时的比电容最高可达1080 F/g,是未功能化石墨烯/聚苯胺电极材料(G/PANI)的2.57倍,且循环稳定性也有很大的提高,循环10000周后的比容量保持率为90.8%,比G/PANI高9.6%.     

NiO/rGO的溶剂热合成以及作为高循环稳定性超级电容器电极材料的性能表征

通过简单的溶剂热法以及其后续热处理过程,制备了NiO纳米花和NiO/还原氧化石墨烯（rGO）复合物。 在NiO/rGO复合物中,rGO作为基底生长NiO,与此同时,NiO则有效的避免了rGO的团聚。 采用热重分析(TG)、场发射扫描电子显微镜(FE-SEM)和X射线衍射对样品的成分、形貌和结构进行了表征。 NiO/rGO复合物（NiO和rGO的质量比为82.7∶17.3）电极呈现优异的电化学性能。 在1 A/g时,初始比电容为514.9 F/g,当材料完全活化后,其比电容高达600 F/g。 同时,在电流密度为10 A/g时,相比于1 A/g时的比电容保持率为83.5%。 此外,该电极材料具有非常优异的循环稳定性,6000次循环后电容衰减率为7.4%。 表明所制备的复合物是一种有应用价值的超级电容器电极材料。     

The effect of the polyaniline morphology on the performance of polyaniline supercapacitors

The polyaniline (PANI) prepared by the pulse galvanostatic method (PGM) or the galvanostatic method on a stainless steel substrate from an aqueous solution of 0.5 mol/l H₂SO₄ with 0.2 mol/l aniline has been studied as an electroactive material in supercapacitors. The electrochemical performance of the PANI supercapacitor is characterized by cyclic voltammetry, a galvanostatic charge–discharge test and electrochemical impedance spectroscopy in NaClO₄ and HClO₄ mixed electrolyte. The results show that PANI films with different morphology and hence different capacitance are synthesized by controlling the synthesis methods and conditions. Owing to the double-layer capacitance and pseudocapacitance increase with increasing real surface area of PANI, the capacitive performances of PANI were enhanced with increasing real surface area of PANI. The highest capacitance is obtained for the PANI film with nanofibrous morphology. From charge–discharge studies of a nanofibrous PANI capacitor, a specific capacitance of 609 F/g and a specific energy density of 26.8 Wh/kg have been obtained at a discharge current density of 1.5 mA/cm². The PANI capacitor also shows little degradation of capacitance after 1,000 cycles. The effects of discharge current density and deposited charge of PANI on capacitance are investigated. The results indicate that the nanofibrous PANI prepared by the PGM is promising for supercapacitors.     

Electrochemical capacitors based on the composite of graphene and nickel foam

An improved Hummers method was developed for the simple and efficient production of high-quality graphene oxide(GO), and the composite of GO and nickel foam(NF)(GO/NF) was fabricated by ultrasonication-vacuum-assisted deposition of an aqueous solution of GO on NF. After chemical or thermal reduction, the composite of reduced GO and nickel foam(r GO/NF) was obtained. The electrochemical capacitance performance of r GO/NF was investigated using cyclic voltammetry and galvanostatic charge/discharge measurements. The chemically reduced r GO/NF composite(C-r GO/NF) exhibited high specific capacitance of 379 F/g at 1.0 A/g and 266.5 F/g at 10 A/g. We also prepared thermally reduced graphene oxide at 473 K in order to illuminate the difference in effect between the chemical and low-temperature thermal reduction methods on electrochemical properties. The cycling performance of thermally reduced r GO/NF composite(T-r GO/NF) and C-r GO/NF had ~91% and ~95% capacitance retention after 2000 cycles in a 6 mol/L KOH electrolyte, respectively. Electrochemical experiments indicated that the obtained r GO/NF has very good capacitive performance and could be used as a potential application of electrochemical capacitors. Our work revealed high electrochemical capacitor performance of r GO/NF composite and provided a facile method of r GO/NF preparation.     

One-pot synthesis of CoO–ZnO/rGO supported on Ni foam for high-performance hybrid supercapacitor with greatly enhanced cycling stability

The high specific capacitance along with good cycling stability are crucial for practical applications of supercapacitors,which always demands high-performance and stable electrode materials.In this work,we report a series of ternary composites of CoO-ZnO with different fractions of reduced graphene oxide(rGO) synthesized by in-situ growth on nickel foam,named as CZG-1,2 and 3,respectively.This sort of binder-free electrodes presents excellent electrochemical properties as well as large capacitance due to their low electrical resistance and high oxygen vacancies.Particularly,the sample of CZG-2(CoO-ZnO/rGO 20 mg) in a nanoreticular structure shows the best electrochemical performance with a maximum specific capacitance of 1951.8 F/g(216.9 mAh/g) at a current intensity of 1 A/g.The CZG-2-based hybrid supercapacitor delivers a high energy density up to 45.9 Wh/kg at a high power density of 800 W/kg,and kept the capacitance retention of 90.1% over 5000 charge-discharge cycles.     

Nickel foam-supported porous NiO/polyaniline film as anode for lithium ion batteries

Nickel foam-supported porous NiO film was prepared by a chemical bath deposition technique, and the NiO/polyaniline (PANI) film was obtained by depositing the PANI layer on the surface of the NiO film. The NiO film was constructed by NiO nanoflakes, and after the deposition of PANI, these nanoflakes were coated by PANI. As an anode for lithium ion batteries, the NiO/PANI film exhibits weaker polarization as compared to the NiO film. The specific capacity after 50 cycles for NiO/PANI film is 520 mAh g⁻¹ at 1 C, higher than that of NiO film (440 mAh g⁻¹). The improvement of these properties is attributed to the enhanced electrical conduction and film stability of the electrode with PANI.