Haskins Justin B, Wu James J, Lawson John W
AMA Inc., Thermal Materials Protection Branch, NASA Ames Research Center, Moffett Field, California 94035, USA.
Photovoltaic and Electrochemical Systems Branch, NASA Glenn Research Center, Cleveland, Ohio 44135, USA.
J Phys Chem C Nanomater Interfaces. 2016 Jun 9;120(22):11993-12011. doi: 10.1021/acs.jpcc.6b02449. Epub 2016 May 24.
We evaluate the influence of Li-salt doping on the dynamics, capacitance, and structure of three ionic liquid electrolytes, [pyr14][TFSI], [pyr13][FSI], and [EMIM][BF], using molecular dynamics and polarizable force fields. In this respect, our focus is on the properties of the electric double layer (EDL) formed by the electrolytes at the electrode surface as a function of surface potential (Ψ). The rates of EDL formation are found to be on the order of hundreds of picoseconds and only slightly influenced by the addition of Li-salt. The EDLs of three electrolytes are shown to have different energy storage capacities, which we relate to the EDL formation free energy. The differential capacitance obtained from our computations exhibits asymmetry about the potential of zero charge and is consistent with the camel-like profiles noted from mean field theories and experiments on metallic electrodes. The introduction of Li-salt reduces the noted asymmetry in the differential capacitance profile. Complementary experimental capacitance measurements have been made on our three electrolytes in their neat forms and with Li-salt. The measurements, performed on glassy carbon electrodes, produce U-like profiles, and Li-salt doping is shown to strongly affect capacitance at high magnitudes of Ψ. Differences in the theoretical and experimental shapes and magnitudes of capacitance are rationalized in terms of the electrode surface and pseudocapacitive effects. In both neat and Li-doped liquids, the details of the computational capacitance profile are well described by Ψ-induced changes in the density and molecular orientation of ions in the molecular layer closest to the electrode. Our results suggest that the addition of Li induces disorder in the EDL, which originates from the strong binding of anions to Li. An in-depth analysis of the distribution of Li in the EDL reveals that it does not readily enter the molecular layer at the electrode surface, preferring instead to be localized farther away from the surface in the second molecular layer. This behavior is validated through an analysis of the free energy of Li solvation as a function of distance from the electrode. Free energy wells are found to coincide with localized concentrations of Li, the depths of which increase with Ψ and suggest a source of impedance for Li to reach the electrode. Finally, we make predictions of the specific energy at ideal graphite utilizing the computed capacitance and previously derived electrochemical windows of the liquids.
我们使用分子动力学和可极化力场,评估了锂盐掺杂对三种离子液体电解质——[pyr14][TFSI]、[pyr13][FSI]和[EMIM][BF]——的动力学、电容和结构的影响。在这方面,我们关注的是电解质在电极表面形成的双电层(EDL)的性质随表面电势(Ψ)的变化情况。发现双电层的形成速率在数百皮秒量级,并且仅受锂盐添加的轻微影响。结果表明,三种电解质的双电层具有不同的储能能力,我们将其与双电层形成自由能联系起来。我们计算得到的微分电容在零电荷电势处呈现不对称性,这与金属电极的平均场理论和实验中观察到的驼峰状曲线一致。锂盐的引入减少了微分电容曲线中观察到的不对称性。我们对三种纯形式的电解质以及添加锂盐后的电解质进行了互补的实验电容测量。在玻璃碳电极上进行的测量产生了U形曲线,并且表明锂盐掺杂在高Ψ值时会强烈影响电容。理论和实验中电容的形状及大小差异可以根据电极表面和赝电容效应来解释。在纯液体和锂掺杂液体中,计算得到的电容曲线细节都可以很好地用Ψ诱导的最靠近电极的分子层中离子密度和分子取向的变化来描述。我们的结果表明,锂的添加会在双电层中引入无序,这源于阴离子与锂的强结合。对双电层中锂分布的深入分析表明,锂不容易进入电极表面的分子层,而是更倾向于定位在离表面较远的第二个分子层中。通过分析锂溶剂化自由能随离电极距离的变化,验证了这种行为。发现自由能阱与锂的局部浓度一致,其深度随Ψ增加,这表明锂到达电极存在阻抗来源。最后,我们利用计算得到的电容和先前推导的液体电化学窗口,对理想石墨上的比能量进行了预测。