Department of Mechanical Engineering, University of California , Santa Barbara, California 93106, United States.
Department of Physiology and Biophysics, Rush University Medical Center , Chicago, Illinois 60612, United States.
Langmuir. 2017 Jun 13;33(23):5642-5651. doi: 10.1021/acs.langmuir.7b00731. Epub 2017 May 30.
In this work we present a systematic study of the lateral (parallel to the wall) and normal (perpendicular to the wall) nanostructure of the electric double layer at a heterogeneous interface between two regions of different surface charges, often found in nanoscale electrochemical devices. Specifically, classical density functional theory (DFT) is used to probe a cation concentration range of 10 mM to 1 M, for valences of +1, + 2, and +3, and a diameter range of 0.15-0.9 nm over widely varying surface charges (between -0.15 and +0.15 C/m). The DFT results predict significant lateral and normal nanostructure in the form of ion concentration oscillations. These results are directly compared with those from Poisson-Boltzmann theory, showing significant deviation between the two theories, not only in the concentration profiles, but also in the sign of the electrostatic potential.
在这项工作中,我们系统地研究了两种不同表面电荷区域之间异质界面处的双电层的横向(平行于壁面)和法向(垂直于壁面)纳米结构,这种异质界面在纳米尺度电化学器件中经常出现。具体而言,我们使用经典密度泛函理论(DFT)来探测阳离子浓度范围为 10 mM 至 1 M、价态为+1、+2 和+3,以及直径范围为 0.15-0.9 nm 的离子,表面电荷范围广泛(在-0.15 到+0.15 C/m2 之间)。DFT 结果预测了以离子浓度振荡形式存在的显著的横向和法向纳米结构。这些结果与泊松-玻尔兹曼理论的结果进行了直接比较,表明两种理论之间存在显著的偏差,不仅在浓度分布上,而且在静电势的符号上。