期刊
ACS NANO
卷 15, 期 7, 页码 11724-11733出版社
AMER CHEMICAL SOC
DOI: 10.1021/acsnano.1c02506
关键词
ionic-liquid supercapacitors; energy storage; ion correlations; ion adsorption; confinement effects; surface transition; nanoporous
类别
资金
- Fundamental Research Funds for the Provincial Universities of Zhejiang [SJLY2020006]
- Foundation of Zhejiang Educational Committee [Y20173 7177]
- Natural Science Foundation of Ningbo [202003N4106]
- K.C.Wong Magna Fund in Ningbo University
- Hong Kong Quantum AI Lab Ltd.
The study found that ion crowding near the electrode surface induced by ion correlations is responsible for the anomalous increase in capacitance as pore size decreases. Reducing ion correlation strength increases capacitance and suppresses the anomalous size dependence. The capacitance peak diverges for a given pore size when the ion correlation strength reaches a critical value, and shifts to smaller pore sizes as the correlation strength decreases.
We investigate the effects of pore size and ion adsorption on the room-temperature ionic liquid capacitor with nanoporous electrodes, with a focus on optimizing the capacitance and energy storage. Using a recently developed modified BSK model accounting for both ion correlations and nonelectrostatic interactions, we find that ion crowding proximate to the electrode surface induced by the spontaneous charge separation due to strong ion correlations is responsible for the anomalous increase in the capacitance with decreasing pore sizes observed in experiments. Reducing the strength of ion correlations increases the capacitance and suppresses the anomalous size dependence. For a given pore size, the capacitance peak diverges when the ion correlation strength a reaches alpha critical value, alpha(sc,L). The capacitance peak shifts to smaller pore size as a decreases because of rapid decrease of alpha(sc,L) with decreasing pore size. Asymmetric preferential ion adsorption is shown to lead to significantly enhanced energy storage close to the transition point for any pore sizes. For a given correlation strength, the energy storage is optimal at a pore size where alpha = alpha(sc,L).
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