4.7 Article

Capacitive energy storage in single-file pores: Exactly solvable models and simulations

Journal

JOURNAL OF CHEMICAL PHYSICS
Volume 155, Issue 17, Pages -

Publisher

AIP Publishing
DOI: 10.1063/5.0066786

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Understanding charge storage in low-dimensional electrodes is crucial for developing novel ecologically friendly devices for capacitive energy storage and conversion and water desalination. We developed a versatile, exactly solvable, one-dimensional off-lattice model for charging single-file pores, which showed excellent quantitative agreement with three-dimensional Monte Carlo simulations. The camel-shaped capacitance appears for strongly ionophilic pores with high ion densities, related to charging mechanisms specific to narrow pores.
Understanding charge storage in low-dimensional electrodes is crucial for developing novel ecologically friendly devices for capacitive energy storage and conversion and water desalination. Exactly solvable models allow in-depth analyses and essential physical insights into the charging mechanisms. So far, however, such analytical approaches have been mainly limited to lattice models. Herein, we develop a versatile, exactly solvable, one-dimensional off-lattice model for charging single-file pores. Unlike the lattice model, this model shows an excellent quantitative agreement with three-dimensional Monte Carlo simulations. With analytical calculations and simulations, we show that the differential capacitance can be bell-shaped (one peak), camel-shaped (two peaks), or have four peaks. Transformations between these capacitance shapes can be induced by changing pore ionophilicity, by changing cation-anion size asymmetry, or by adding solvent. We find that the camel-shaped capacitance, characteristic of dilute electrolytes, appears for strongly ionophilic pores with high ion densities, which we relate to charging mechanisms specific to narrow pores. We also derive a large-voltage asymptotic expression for the capacitance, showing that the capacitance decays to zero as the inverse square of the voltage, C & SIM; u(-2). This dependence follows from hard-core interactions and is not captured by the lattice model.

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