Department of Materials Science & Engineering, University of Utah, 122 S. Central Campus Drive, Rm 304, Salt Lake City, Utah 84112, USA.
J Phys Chem B. 2012 Oct 25;116(42):12801-9. doi: 10.1021/jp3052246. Epub 2012 Oct 11.
Molecular dynamics simulations of N-methyl-N-propylpyrrolidinium (pyr(13)) bis(trifluoromethanesulfonyl)imide (Ntf(2)) ionic liquid [pyr(13)][Ntf(2)] mixed with [Li][Ntf(2)] salt have been conducted using a polarizable force field. Mixture simulations with lithium salt mole fractions between 0% and 33% at 363 and 423 K yield densities, ion self-diffusion coefficients, and ionic conductivities in very good agreement with available experimental data. In all investigated electrolytes, each Li(+) cation was found to be coordinated, on average, by 4.1 oxygen atoms from surrounding anions. At lower concentrations (x ≤ 0.20), the Li(+) cation was found to be, on average, coordinated by slightly more than three Ntf(2) anions with two anions contributing a single oxygen atom and one anion contributing two oxygen atoms to Li(+) coordination. At the highest [Li][Ntf(2)] concentration, however, there were, on average, 3.5 anions coordinating each Li(+) cation, corresponding to fewer bidendate and more monodentate anions in the Li(+) coordination sphere. This trend is due to increased sharing of anions by Li(+) at higher salt concentrations. In the [pyr(13)][Ntf(2)]/[Li][Ntf(2)] electrolytes, the ion diffusivity is significantly smaller than that in organic liquid electrolytes due to not only the greater viscosity of the solvent but also the formation of clusters resulting from sharing of anions by Li(+) cations. The ionic conductivity of the electrolytes was found to decrease with increasing salt concentration, with the effect being greater at the higher temperature. Finally, we found that the contribution of Li(+) to ionic conductivity does not increase proportionally to Li(+) concentration but saturates at higher doping levels.
采用极化力场对 N-甲基-N-丙基吡咯烷(pyr(13))双(三氟甲烷磺酰基)亚胺(Ntf(2))离子液体 [pyr(13)][Ntf(2)] 与 [Li][Ntf(2)] 盐的混合物进行了分子动力学模拟。在 363 和 423 K 下,锂盐摩尔分数在 0% 到 33% 之间的混合模拟得到的密度、离子自扩散系数和离子电导率与可用的实验数据非常吻合。在所研究的所有电解质中,每个 Li(+)阳离子平均被周围阴离子的 4.1 个氧原子配位。在较低浓度(x ≤ 0.20)下,Li(+)阳离子平均被略多于三个 Ntf(2)阴离子配位,其中两个阴离子提供一个氧原子,一个阴离子提供两个氧原子给 Li(+)配位。然而,在最高 [Li][Ntf(2)]浓度下,每个 Li(+)阳离子平均有 3.5 个阴离子配位,这对应于 Li(+)配位球中更少的双齿和更多的单齿阴离子。这种趋势是由于在较高盐浓度下 Li(+)共享阴离子的增加。在 [pyr(13)][Ntf(2)]/[Li][Ntf(2)]电解质中,离子扩散率显著小于有机溶剂电解质中的扩散率,这不仅是由于溶剂的粘度较大,而且还由于 Li(+)阳离子共享阴离子导致形成了聚集体。电解质的离子电导率随着盐浓度的增加而降低,在较高温度下,这种影响更大。最后,我们发现 Li(+)对离子电导率的贡献并不随 Li(+)浓度成比例增加,而是在较高掺杂水平下饱和。