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Molecular Insights into the Potential and Temperature Dependences of the Differential Capacitance of a Room-Temperature Ionic Liquid at Graphite Electrodes

机译:室温离子液体在石墨电极上的微分电容的电位和温度依赖性的分子洞察力

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摘要

Molecular dynamics simulation studies of the structure and the differential capacitance (DC) for the ionic liquid (IL) N-methyl-N-propylpyrrolidinium bis(trifluoromethane)sulfonyl imide ([pyr13][TFSI]) near a graphite electrode have been performed as a function temperature and electrode potential. The IL exhibits a multilayer structure that extends 20−30 Å from the electrode surface. The composition and ion orientation in the innermost layer were found to be strongly dependent on the electrode potential. While at potentials near the potential of zero charge (PZC), both cations and anions adjacent to the surface are oriented primarily perpendicular to the surface, the counterions in first layer orient increasingly parallel to the surface with increasing electrode potential. A minimum in DC observed around −1 VRPZC (potential relative to the PZC) corresponds to the point of highest density of perpendicularly aligned TFSI near the electrode. Maxima in the DC observed around +1.5 and −2.5 VRPZC are associated with the onset of “saturation”, or crowding, of the interfacial layer. The asymmetry of DC versus electrode polarity is the result of strong interactions between the fluorine of TFSI and the surface, the relatively large footprint of TFSI compared to pyr13, and the tendency of the propyl tails of pyr13 to remain adsorbed on the surface even at high positive potentials. Finally, an observed decreased DC and the disappearance of the minimum in DC near the PZC with increasing temperature are likely due to the increasing importance of entropic/excluded volume effects (interfacial crowding) with increasing temperature.
机译:离子液体(IL)N-甲基-N-丙基吡咯烷鎓双(三氟甲烷)磺酰酰亚胺([pyr 13 ] [TFSI])的结构和微分电容(DC)的分子动力学模拟研究已经将石墨电极附近的温度作为函数温度和电极电位。 IL表现出从电极表面延伸20-30Å的多层结构。发现最内层中的组成和离子取向强烈依赖于电极电势。当处于接近零电荷(PZC)电位的电位时,与表面相邻的阳离子和阴离子都主要垂直于表面,而第一层中的抗衡离子随着电极电位的增加而逐渐平行于表面。在-1 V RPZC 附近观察到的最小直流电压(相对于PZC的电位)对应于电极附近垂直排列的TFSI的最高密度点。在+1.5和-2.5 V RPZC 附近观察到的DC最大值与界面层“饱和”或拥挤有关。 DC与电极极性的不对称性是由于TFSI的氟与表面之间的强相互作用,TFSI与pyr 13 相比具有相对较大的占位面积以及pyr < sub> 13 即使在高正电势下也保持吸附在表面上。最后,随着温度升高,观察到的DC降低以及PZC附近DC最小值的消失很可能是由于熵/排除体积效应(界面拥挤)随着温度升高而变得越来越重要。

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  • 来源
    《Journal of the American Chemical Society》 |2010年第42期|p.14825-14833|共9页
  • 作者单位

    Department of Materials Science and Engineering, University of Utah, Salt Lake City, Utah 84112, United States;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-18 00:50:27

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