首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到18条相似文献,搜索用时 125 毫秒
1.
以(NH4)2S2O8为氧化剂,通过化学氧化法在TiO2颗粒表面包覆聚苯胺(PANI)薄膜制得PANI/TiO2。通过静电自组装方法将SiW412-键合在PANI/TiO2表面,制备了一种新型的复合光催化剂PANI/TiO2/SiW12(1),用UV-Vis,FT-IR,XRD和SEM等对1的结构和光吸收性能进行了表征。以刚果红为目标降解物,研究了1在太阳光下的光催化性能。结果表明,PANI的敏化作用拓宽了TiO2的光响应范围,提高了光能的利用率,增强了复合材料的光催化活性。1的光催化活性明显高于TiO2和PANI/TiO2,90 min降解率达83.94%。  相似文献   

2.
利用层层自组装技术,将聚丙烯酸修饰的石墨烯(PAA-Gr)与聚苯胺(PANI)进行层层自组装,制备了石墨烯/聚苯胺{PAA-Gr/PANI}n复合薄膜.聚丙烯酸修饰石墨烯不仅可以提高石墨烯的分散性,而且可以使石墨烯表面带负电荷,为其与带正电的PANI进行层层自组装提供了可能.利用紫外光谱跟踪了{PAA-Gr/PANI}n复合薄膜层层自组装过程.通过红外光谱、X射线衍射、扫描电子显微镜和循环伏安等方法表征了{PAA-Gr/PANI}n复合薄膜的结构.研究了{PAA-Gr/PANI}n复合薄膜的电化学性能,并探讨了复合薄膜在过氧化氢(H2O2)传感器中的应用.{PAA-Gr/PANI}n复合薄膜对H2O2表现出良好的电催化活性,其线性检测范围为0.005~0.3 mmol/L,线性相关系数为0.99858,检测下限为1×10-6mol/L.  相似文献   

3.
采用具有八面体形貌的氧化亚铜为模板,制备了聚苯胺/TiO2(PANI/TiO2)微/纳米球,TiO2纳米粒子很均匀地分散在聚苯胺中.研究了不同TiO2/苯胺(TiO2/ANI)摩尔比对PANI/TiO2复合物的结构、形貌和电学性能的影响.实验结果表明,随着TiO2/ANI摩尔比的增加,PANI/TiO2复合物的直径逐渐减小,当TiO2/ANI摩尔比为0.16时,复合物的平均直径为373nm,而当TiO2/ANI摩尔比增加到1.6时,复合物的平均直径降到80nm.PANI/TiO2复合微/纳米球的电导率随着TiO2/ANI摩尔比的增加先升高后降低,当TiO2/ANI摩尔比达到1.6时,电导率由10-4S/cm提高到100S/cm,达到最大值.产物的形貌和结构分别采用扫描电镜、透射电镜、红外吸收光谱和X-射线衍射等手段进行了表征.  相似文献   

4.
TiO_2聚苯胺复合膜的光电化学   总被引:15,自引:2,他引:13  
利用电化学方法制备了TiO2 聚苯胺 (PANI)复合膜 .该膜具有比TiO2 或PANI膜更宽的吸收谱区 ,并且不同于利用聚苯胺光敏化的TiO2 膜 ,表现为两者复合材料膜的性质 .扫描电镜图表明 ,TiO2 微粒不完全覆盖着PANI膜 .根据TiO2 微粒光电流谱带的阈值能可得复盖在部分氧化态聚苯胺膜上的TiO2 微粒的禁带宽度为 3.0eV .部分氧化态聚苯胺膜的光电流谱遵循Fowler定律 ( 1/2 ~hυ成线性 ) .通过Fowler图得出部分氧化态聚苯胺的绝缘母体禁带宽度为 3.33eV ,并证实该绝缘母体为还原态聚苯胺 .从Mott Schottky图得到在 0 .0 5mol/LK3Fe(CN) 6 /K4 Fe(CN) 6 溶液中 (pH =8.52 )部分氧化态聚苯胺的平带电位为 0 .13V ,掺杂浓度为 5.3× 10 18cm- 3;TiO2 PANI复合膜的平带电位为 - 0 .6 5V ,掺杂浓度为 9.1× 10 19cm- 3.解释了TiO2 PANI复合膜的光电化学过程并描绘出其能带图 .利用TiO2 PANI复合膜能够有效地光降解苯酚溶液 .  相似文献   

5.
采用水解胶溶法和旋转涂膜法分别制备出TiO2纳米粒子溶胶和TiO2/ITO薄膜, 采用浸泡法制备出苯封四聚苯胺(聚苯胺)/TiO2/ITO薄膜电极. 利用表面光电压谱、光致循环伏安和光电流作用谱测定了TiO2的禁带宽度和表面态能级、聚苯胺的 HOMO-LUMO能级宽度和双极化子能级, 确定了聚苯胺/TiO2/ITO薄膜电极能带结构. 进一步分析了聚苯胺/TiO2/ITO薄膜电极的光电转换特性及光致界面电荷转移的机理.  相似文献   

6.
应用电化学方法在不同条件下制备聚苯胺 (PANI)膜和TiO2 -PANI复合膜 ,并对其光电化学性能进行研究 .实验表明 ,制备条件是影响膜光电化学性能的重要因素 .对氨基硫酚 (PATP)的组装有利于改善PANI膜的附着力 ;部分氧化态PANI膜的光电化学响应明显优于还原态和氧化态PANI膜的光电化学响应 ;部分氧化态PANI膜的厚度对其光电化学性能有一最佳值 ;热处理虽然有利于改善TiO2 的光电化学性能 ,但温度太高 ,将破坏PANI膜的表面结构 ,对于TiO2 -PANI复合膜有一最佳的热处理温度 .优化制备条件大可改善TiO2 -PANI复合膜和PANI膜的光电化学性能  相似文献   

7.
提出了一种基于溶液表面的聚苯胺(PANI)薄膜及气敏器件的室温制备方法,以苯胺单体、盐酸和过硫酸铵为原料通过氧化聚合在其水溶液表面直接获得质子化聚苯胺(PANI)薄膜,并利用薄膜的可转移特性构筑气敏器件.研究发现溶液的pH对PANI致密薄膜的形成至关重要,从而提出了质子化苯胺单体优先在溶液表面聚集和聚合的PANI薄膜形成机制.该薄膜气敏器件能够对NH3进行有效的室温检测,且性能随薄膜聚合温度和聚合时间的变化呈规律性变化,优选制备条件下(pH=0.6,室温18℃,聚合60 min)的薄膜其检测下限为10-6,响应与NH3浓度呈良好的线性关系,并具有良好的重复性、选择性、快速响应和有竞争力的响应值.该薄膜制备工艺体现了“绿色”制备思想,且薄膜能够大面积制备并具有优异的气敏性能,有望为PANI-基薄膜的制备与室温气体传感器的研究与应用提供一种新的思路.  相似文献   

8.
首先用偶联剂苯胺基甲基三乙氧基硅烷(AMTES)对纳米TiO2进行表面修饰(AMTES-TiO2), 然后通过苯胺单体在AMTES-TiO2表面的原位化学氧化接枝聚合, 制备了基于共价键结合的聚苯胺(PANI)/AMTES-TiO2纳米复合光催化材料. 用红外光谱(FTIR), X射线衍射(XRD), 热重分析(TGA), 紫外-可见漫反射光谱(UV-Vis-DRS)和荧光发射光谱(PL)等技术对复合材料进行了表征. 以亚甲基蓝(MB)为目标降解物, 研究了PANI/AMTES-TiO2复合材料在太阳光和紫外光下的光催化性能. 结果表明:聚苯胺敏化拓宽了TiO2的光谱响应范围, 复合材料在紫外和可见光区都有较强的吸收, 提高了光能的利用率和光生载流子的分离效率, 使复合材料表现出较高的光催化活性; 苯胺与AMTES-TiO2的质量比(w)对复合材料的光催化活性有较大影响, 当w为0.025时, 复合材料在两种光源下的催化性能均优于TiO2和AMTES-TiO2.  相似文献   

9.
首先用偶联剂苯胺基甲基三乙氧幕硅烷(AMTES)对纳米TiO2进行表而修饰(AMTES-TiO2),然后通过苯胺单体在AMTES-TiO2表面的原位化学氧化接枝聚合,制备了基于共价键结合的聚苯胺(PANI)/AMTES-TiO2纳米复合光催化材料.用红外光谱(FTIR),X射线衍射(XRD),热重分析(TGA),紫外-可见漫反射光谱(UV-Vis-DRS)和荧光发射光谱(PL)等技术对复合材料进行了表征.以亚甲基蓝(MB)为目标降解物,研究了 PANI/AMTES-TiO2复合材料在太阳光和紫外光下的光催化性能.结果表明:聚苯胺敏化拓宽了TiO2的光谱响应范围,复合材料在紫外和可见光区都有较强的吸收,提高了光能的利用率和光生载流子的分离效率,使复合材料表现出较高的光催化活性;苯胺与AMTES-TiO2的质量比(w)对复合材料的光催化活性有较大影响,当w为0.025时,复合材料在两种光源下的催化性能均优于TiO2和AMTES-TiO2.  相似文献   

10.
Pt微粒修饰纳米纤维聚苯胺电极对甲醇氧化电催化   总被引:9,自引:0,他引:9  
以脉冲电流法制备的纳米纤维状聚苯胺(PANI)为Pt催化剂载体,用它制备了甲醇阳极氧化的催化电极Pt/(nano-fibular PANI).研究结果表明, Pt/(nano-fibular PANI)电极对甲醇氧化具有很好的电催化活性,并有协同催化作用.在相同的Pt载量条件下, Pt/(nano-fibular PANI)电极比Pt微粒修饰的颗粒状聚苯胺电极Pt/(granular PANI)具有更好的电催化活性.此外, Pt的电沉积修饰方法同样影响Pt/(nano-fibular PANI)电极对甲醇氧化的催化活性.脉冲电流法沉积Pt形成的复合电极较循环伏安法电沉积得到的Pt复合电极具有更优异的催化活性.  相似文献   

11.
We present novel nanoporous TiO(2)/polyion thin-film-coated long-period fiber grating (LPFG) sensors for the direct measurement of low-molecular-weight chemicals by monitoring the resonance wavelength shift. The hybrid overlay films are prepared by a simple layer-by-layer deposition approach, which is mainly based on the electrostatic interaction of TiO(2) nanoparticles and polyions. By the alternate immersion of LPFG into dispersions of TiO(2) nanoparticles and polyions, respectively, the so-formed TiO(2)/polyion thin film exhibits a unique nanoporous internal structure and has a relative higher refractive index than LPFG cladding. In particular, the porosity of the thin film reduces the diffusion coefficient and enhances the permeability retention of low-molecular-weight analytes within the porous film. The increases in the refractive index of the LPFG overlay results in a distinguished modulation of the resonance wavelength. Therefore, the detection sensitivity of LPFG sensors has been greatly improved, according to theoretical simulation. After the structure of the TiO(2)/polyion thin film was optimized, glucose solutions as an example with a low concentration of 10(-7) M was easily detected and monitored at room temperature.  相似文献   

12.
室温下通过电泳沉积(EPD)的方法在Ti片表面制备TiN薄膜, 然后对TiN薄膜进行阳极氧化得到N掺杂多孔纳米结构的TiO2薄膜. 利用X射线衍射(XRD), X射线光电子能谱(XPS), 扫描电子显微镜(SEM)及光电化学方法对得到的薄膜进行表征. XRD测试结果表明, 经过阳极氧化并在350 ℃空气气氛中退火1 h的薄膜中存在锐钛矿晶型的TiO2. XPS的结果表明, 样品中的N元素取代部分O, 且N的摩尔分数为0.95%. SEM显示, 经阳极氧化后薄膜表面出现多孔纳米结构. 光电化学测试结果显示, 阳极氧化提高了N掺杂TiO2薄膜在可见光下的光电响应. 经阳极氧化并热处理的薄膜在0 V电位及可见光照射下光电流密度为2.325 μA·cm-2, 而单纯热处理的薄膜在相同条件下光电流密度仅为0.475 μA·cm-2. 阳极氧化得到纳米多孔结构提高了N掺杂纳米TiO2薄膜的表面积, 从而对可见光的响应增大.  相似文献   

13.
通过阳极氧化的方法制备TiO2纳米管薄膜, 在MoO3存在的条件下对该薄膜进行热处理得到TiO2-MoO3复合纳米管阵列薄膜. 利用X射线衍射(XRD), 扫描电子显微镜(SEM), X射线光电子能谱(XPS), 电化学阻抗谱(EIS), Mott-Schottky 及光电化学方法对得到的薄膜进行了表征. XRD结果表明, TiO2-MoO3复合纳米管薄膜中的TiO2主要为锐钛矿晶型. SEM实验证实了薄膜纳米管结构的存在, 样品中的MoO3均匀地分散在TiO2纳米管表面. 利用XPS方法分析了TiO2-MoO3复合纳米管薄膜元素的组成, 结果表明, MoO3在TiO2表面形成TiO2-MoO3复合纳米管薄膜. 研究了热处理温度以及热处理时间对样品的光电化学性能的影响, 相对于单纯TiO2纳米管薄膜, 适量引入MoO3提高了样品在可见光区的光电响应能力, 样品的平带电位负移. 在450 °C热处理60 min制得的TiO2-MoO3复合半导体纳米管阵列薄膜光电响应活性最高.  相似文献   

14.
The gas separation properties of free- standing film of polyaniline (PANI) for gas pairs of He/N2, H_2/N_2. CO_2/N_2 and CO_2/CH_4 at room temperature were measured as a function of the protonation state. Variation of the gas permeabilities coefficient of PANI with an insulator to metal transition upon the protonation processes was observed, which might be due to a change in both gas solubility coefficient and diffusion coefficient with the protonation state.  相似文献   

15.
The charge transport properties of thin films prepared from colloidal dispersion of polyaniline stabilized by poly(N‐vinylpyrrolidone) (PANI/PVP) have been investigated. The electrical characterization of coplanar device comprising of gold electrodes and PANI/PVP film deposited by spin coating served to gain insights into the contact and bulk resistance. The films prepared from PANI/PVP colloidal dispersion show high stability over a large temperature range. Temperature dependent measurements in the range from 90 to 350 K reveal that the charge transport can be described by a three‐dimensional variable‐range hopping mechanism as the dominant mode in the films. The stability of the films cast from dispersion within a large temperature range opens the possibility of the application as a polymer semiconductor layer in sensors and charge‐transport interlayer in organic solar cells. © 2016 Wiley Periodicals, Inc. J. Polym. Sci., Part B: Polym. Phys. 2016 , 54, 1710–1716  相似文献   

16.
Nanocrystalline TiO2 thin films composed of densely packed grains were deposited onto indium-doped tin oxide (ITO)-coated glass substrates at room temperature using a chemical bath deposition technique. A layer-by-layer (LbL) process was utilized to obtain a 1.418-microm-thick TiO2/ZnO structure. The TiO2 surface was super-hydrophilic, but its hydrophilicity decreased considerably after ZnO deposition. Other TiO2/ZnO films were studied to assess their suitability as photoelectrodes in dye-sensitized solar cells (DSSCs).  相似文献   

17.
Polyaniline (PANI) films were deposited by electrochemical polymerization of aniline monomer on a fluorine-doped glass substrate at room temperature under different electric field directions. The as-synthesized PANI films obtained at different growth cycles were characterized by AC impedance spectroscopy and scanning electron microscopy (SEM). The results revealed that the film morphology, transport kinetics, and electrical properties are strongly dependent on the electric field direction and magnitude of the applied field during electropolymerization. The SEM morphology and AC impedance (modulus spectroscopy) indicate that a more homogeneous, high-porous, and conducting PANI film is induced by horizontal electric field direction (HEFD) electrodeposition, whereas the modulus spectroscopy of the PANI film deposited by vertical electric field direction (VEFD) reveals that VEFD deposition favours two-dimensional growth of PANI. The obtained polymer is more of dielectric in nature due to preferable dendritic growth which is supported by SEM analysis.  相似文献   

18.
We report on the photoinduced superhydrophilicity of the surface of amorphous TiO2. Amorphous TiO2 thin films were prepared on self-assembled monolayers by the peroxotitanate-complex deposition (PCD) and liquid-phase deposition (LPD) methods. The surface morphology and topography were characterized in detail. The contact angles were 34 degrees and 66 degrees for the as-deposited thin films through the PCD and LPD methods, respectively, which slowly increased to about 70 degrees and 73 degrees after being stored in air. After irradiation by UV light, the contact angle vanished and the surface exhibited superhydrophilicity. The superhydrophilicity and hydrophobicity could be switched by alternatively exposing the surface to UV light and drying in an atmosphere filled with organic gases. Although the oxidation of the contamination on the surface has effects on the increase in hydrophilicity, the X-ray photoelectron spectroscopy results suggested that the superhydrophilicity was also related to the transformation of the Ti-OH groups to groups that have dangling bonds. This paper indicates that an amorphous TiO2 thin film does not need to be heated to obtain superhydrophilicity; such a self-cleaning surface can be achieved at room temperature by our newly developed environmentally friendly method.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号