Department of Materials Science and Engineering, University of Utah, Salt Lake City, Utah 84112, USA.
J Phys Chem B. 2011 Mar 31;115(12):3073-84. doi: 10.1021/jp2001207. Epub 2011 Mar 8.
Molecular dynamics simulations were performed on N-methyl-N-propylpyrrolidinium bis(fluorosulfonyl)imide (pyr(13)FSI) room temperature ionic liquid (RTIL) confined between graphite electrodes as a function of applied potential at 393 and 453 K using an accurate force field developed in this work. The electric double layer (EDL) structure and differential capacitance (DC) of pyr(13)FSI was compared with the results of the previous study of a similar RTIL pyr(13)bis(trifluoromethanesulfonyl)imide (pyr(13)TFSI) with a significantly larger anion [ Vatamanu, J.; Borodin, O.; Smith, G. D. J. Am. Chem. Soc. 2010, 132, 14825]. Intriguingly, the smaller size of the FSI anion compared to TFSI did not result in a significant increase of the DC on the positive electrode. Instead, a 30% higher DC was observed on the negative electrode for pyr(13)FSI compared to pyr(13)TFSI. The larger DC observed on the negative electrode for pyr(13)FSI compared to pyr(13)TFSI was associated with two structural features of the EDL: (a) a closer approach of FSI compared to TFSI to the electrode surface and (b) a faster rate (vs potential decrease) of anion desorption from the electrode surface for FSI compared to TFSI. Additionally, the limiting behavior of DC at large applied potentials was investigated. Finally, we show that constant potential simulations indicate time scales of hundreds of picoseconds required for electrode charge/discharge and EDL formation.
采用本工作中开发的精确力场,对 N-甲基-N-丙基吡咯烷双(氟磺酰基)亚胺(pyr(13)FSI)室温离子液体(RTIL)在 393 和 453 K 下于施加电势下在石墨电极之间进行了分子动力学模拟。与先前对具有较大阴离子的类似 RTIL pyr(13)双(三氟甲磺酰基)亚胺(pyr(13)TFSI)的研究结果相比,比较了 pyr(13)FSI 的双电层(EDL)结构和微分电容(DC)[Vatamanu, J.; Borodin, O.; Smith, G. D. J. Am. Chem. Soc. 2010, 132, 14825]。有趣的是,FSI 阴离子的尺寸小于 TFSI 并没有导致 DC 在正极上显著增加。相反,与 pyr(13)TFSI 相比,在负极上观察到 pyr(13)FSI 的 DC 增加了 30%。与 pyr(13)TFSI 相比,在负极上观察到的 pyr(13)FSI 的较大 DC 与 EDL 的两个结构特征有关:(a)FSI 比 TFSI 更接近电极表面,(b)FSI 比 TFSI 从电极表面更快地(相对于电势降低)脱附阴离子。此外,研究了大施加电势下 DC 的极限行为。最后,我们表明,恒电位模拟表明电极充电/放电和 EDL 形成所需的时间尺度为数百皮秒。