Issue |
EPL
Volume 140, Number 1, October 2022
|
|
---|---|---|
Article Number | 16001 | |
Number of page(s) | 7 | |
Section | Condensed matter and materials physics | |
DOI | https://doi.org/10.1209/0295-5075/ac9252 | |
Published online | 27 September 2022 |
Electrosorption-induced deformation of a porous electrode with non-convex pore geometry in electrolyte solutions: A theoretical study
1 Institut für Nichtklassische Chemie e.V. - Permoserstr. 15, 04318 Leipzig, Germany
2 School of Applied Mathematics, HSE University - Tallinskaya st. 34, 123458 Moscow, Russia
3 G.A. Krestov Institute of Solution Chemistry of the Russian Academy of Sciences 153045, Akademicheskaya st. 1, Ivanovo, Russia
(a) E-mail: kolesnikov@inc.uni-leipzig.de (corresponding author)
Received: 7 June 2022
Accepted: 15 September 2022
Porous carbon is well known as a good candidate for the development of electrochemical double-layer capacitors. Predominantly, many conventional carbons are microporous and often well described by the assumption of slit pore geometry. However, there is a class of carbons that is significantly different from the others, namely templated mesoporous carbons. In this work, we study electrosorption-induced deformation in CMK-3–like mesopores having non-convex geometry. Our mean-field approach is based on the modified Poisson-Boltzmann equation taking into account the excluded volume of the ions within the hard-sphere model. We assume that the deformation is caused by two effects: ion osmotic pressure and electrostatic interactions of the electric double layers on charged rods. We estimated the pore-load modulus of the CMK-3–like material and found an agreement with the previously obtained values by small-angle neutron scattering (SANS) data analysis. Additionally, we studied the differential capacitance in the non-convex pore geometry and found that the behavior of the differential capacitance profiles was similar to that of the profiles obtained for flat electric double layers: the crowding regime at rather high electric potentials and more pronounced profile asymmetry with increasing differences in the ionic sizes.
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