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Effect of an Iodine Film on Charge-Transfer Resistance during the Electro-Oxidation of Iodide in Redox Flow Batteries

35

Citations

28

References

2021

Year

Abstract

The use of iodide as the positive redox-active species in redox flow batteries has been highly anticipated owing to its attractive features of high solubility, excellent reversibility, and low cost. However, the electro-oxidation reaction of iodide (I<sup>-</sup>) is very complicated, giving various possible products such as iodine (I<sub>2</sub>), polyiodides (I<sub>2<i>n</i>+1</sub><sup>-</sup>), and polyiodines (I<sub>2<i>n</i>+2</sub>) with <i>n</i> ≥ 1. In particular, the electro-oxidation of I<sup>-</sup>/I<sub>3</sub><sup>-</sup> and I<sub>3</sub><sup>-</sup>/I<sub>2</sub> occurs in competition depending on the applied potential. Although the former reaction is adopted as the main reaction in most redox flow batteries because I<sub>3</sub><sup>-</sup> is highly soluble in an aqueous electrolyte, the latter reaction inevitably occurs together and a thick I<sub>2</sub>-film forms on the electrode, impeding the electro-oxidation of I<sup>-</sup>. In this study, we investigate the variation of the interface between the electrode and the electrolyte during the development of an I<sub>2</sub>-film and the corresponding change in the charge-transfer resistance (<i>R</i><sub>ct</sub>). Initially, the I<sub>2</sub>-film builds upon the electrode surface in the form of a porous layer and the aqueous I<sup>-</sup> ions can easily reach the electrode surface through pores inside the film. I<sup>-</sup> ions are electro-oxidized to I<sub>3</sub><sup>-</sup> or I<sub>2</sub> at the interface between the aqueous I<sup>-</sup> phase and electrode with a small <i>R</i><sub>ct</sub> of less than 16.5 ohm·cm<sup>2</sup>. Over time, the I<sub>2</sub>-film is converted into a dense layer and I<sup>-</sup> ions diffuse through the film in the form of I<sub>3</sub><sup>-</sup>, possibly by a Grotthuss-type hopping mechanism. I<sub>3</sub><sup>-</sup> can then be electro-oxidized to I<sub>2</sub> at the new interface between the I<sub>2</sub>-film and electrode, resulting in a dramatic 9-fold increase of <i>R</i><sub>ct</sub> to 147.4 ohm·cm<sup>2</sup>. This increase of <i>R</i><sub>ct</sub> by the dense I<sub>2</sub>-film is also observed in the actual flow battery. At high current densities above 400 mA·cm<sup>-2</sup>, the overpotential begins to show an abrupt increase in the amplitude of more than 300 mV after reaching a critical charging capacity at which the dense I<sub>2</sub>-film appears to have begun to form on the felt electrode. Therefore, the I<sub>2</sub>-film exerts a serious negative effect on the performance of the flow battery depending on the current density and electrolyte SoC (state-of-charge).

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