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Structure and Capacitance of Electrical Double Layers at the Graphene–Ionic Liquid Interface

机译:石墨烯-离子液体界面的双电层的结构和电容

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Molecular dynamics simulations are carried out to investigate the structure and capacitance of the electrical double layers (EDLs) at the interface of vertically oriented graphene and ionic liquids [EMIM] + /[BF 4 ] ? . The distribution and migration of the ions in the EDL on the rough and non-rough electrode surfaces with different charge densities are compared and analyzed, and the effect of the electrode surface morphology on the capacitance of the EDL is clarified. The results suggest that alternate distributions of anions and cations in several consecutive layers are formed in the EDL on the electrode surface. When the electrode is charged, the layers of [BF 4 ] ? anions experience more significant migration than those of [EMIM] + cations. These ion layers can be extended deeper into the bulk electrolyte solution by the stronger interaction of the rough electrode, compared to those on the non-rough electrode surface. The potential energy valley of ions on the neutral electrode surface establishes a potential energy difference to compensate the energy cost of the ion accumulation, and is capable of producing a potential drop across the EDL on the uncharged electrode surface. Due to the greater effective contact area between the ions and electrode, the rough electrode possesses a larger capacitance than the non-rough one. In addition, it is harder for the larger-sized [EMIM] + cations to accumulate in the narrow grooves on the rough electrode, when compared with the smaller [BF 4 ] ? . Consequently, the double-hump-shaped C–V curve (which demonstrates the relationship between differential capacitance and potential drop across the EDL) for the rough electrode is asymmetric, where the capacitance increases more significantly when the electrode is positively charged.
机译:进行分子动力学模拟以研究在垂直取向的石墨烯和离子液体[EMIM] + / [BF 4]的界面处的双电层(EDL)的结构和电容。 。比较和分析了不同电荷密度下粗糙和非粗糙电极表面上EDL中离子的分布和迁移,并阐明了电极表面形态对EDL电容的影响。结果表明,在电极表面的EDL中形成了多个连续层中阴离子和阳离子的交替分布。当电极带电时,[BF 4]→SiO 2层。阴离子比[EMIM] +阳离子迁移更为显着。与非粗糙电极表面上的离子层相比,通过粗糙电极之间更强的相互作用,这些离子层可以更深地扩展到整体电解质溶液中。中性电极表面上离子的势能谷建立势能差以补偿离子累积的能量成本,并能够在不带电电极表面上的EDL两端产生电势降。由于离子与电极之间的有效接触面积更大,因此粗糙电极比非粗糙电极具有更大的电容。另外,与较小的[BF 4]相比,较大的[EMIM] +阳离子难以积聚在粗糙电极的狭窄槽中。 。因此,粗糙电极的双峰状C–V曲线(证明了差分电容和EDL两端电位降之间的关系)是不对称的,当电极带正电时,电容会显着增加。

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