Bubble Dynamics in Photoelectrochemical Water Splitting Cell at Elevated Pressure
Feng Liang a, Roel van de Krol a, Fatwa Firdaus Abdi a
a Institute for Solar Fuels, Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Hahn-Meitner-Platz 1, 14109 Berlin, Germany
Materials for Sustainable Development Conference (MATSUS)
Proceedings of MATSUS Fall 2023 Conference (MATSUSFall23)
#NextED - Next generation of electrochemical devices
Torremolinos, Spain, 2023 October 16th - 20th
Organizers: Moritz Futscher and Angus Mathieson
Poster, Feng Liang, 221
Publication date: 18th July 2023

Photoelectrochemical (PEC) water splitting is one of the few truly renewable pathways towards “green” H2. Operating PEC water splitting at elevated pressure offers many benefits. For example, bubble formation is strongly reduced at elevated pressure, which lowers bubble-induced electrode deactivation and bubble-induced product crossover rate.[1,2] In addition, the optical reflection and diffraction losses induced by bubbles can be minimized.[3] Finally, the electrochemical production of hydrogen at higher pressure requires only a small (though not insignificant) increase of the thermodynamic cell voltage (29 mV for 10-fold increase in pressure).[4] However, bubble dynamics in a photoelectrochemical cell at elevated pressure, e.g. bubble diameter and bubble coverage on the photoelectrode, remain unclear, therefore need to be investigated. In this work, we conducted a shadowgraphy study on galvanostatically formed O2 bubbles in a pressurized (1-4 bar) PEC water splitting cell, as shown schematically in Fig. 1a. BiVO4 was electrochemically prepared on an FTO substrate and used as the anode, with Pt wire and a leak-less Ag/AgCl as the cathode and reference electrode, respectively. The electrolyte was 0.1 M potassium borate buffer (KBi, pH9). As shown in Fig. 1b, an instant drop in cell potential was observed while elevating the cell pressure from 1 bar to 2 bar. Using bubble shadowgraphy (Fig. 1c), we could correlate this cell potential drop with the shrinkage of bubble diameter. Interestingly, further pressurizations, i.e. from 2 bar to 3 bar and from 3 bar to 4 bar, led to only minor changes in both the cell potential and bubble diameter. The quantitative impact of this observation with respect to the various loss mechanism in a PEC cell (e.g. thermodynamic, optical loss, product crossover, activation) will be discussed. Overall, the findings from this work serve as a guideline in designing highly efficient photoelectrochemical water splitting cell at elevated pressure.

The Helmholtz Association of German Research Centers (HGF) and the Federal Ministry of Education and Research (BMBF), Germany are gratefully acknowledged for supporting the development of solar powered technologies for H2 generation within the frame of the Innovation Pool project “Solar H2: Highly Pure and Compressed” and the Helmholtz Research Program “Materials and Technologies for the Energy Transition” (MTET). Part of the work was also carried out with the support of the Helmholtz Energy Materials Foundry (HEMF), a large-scale distributed research infrastructure founded by the German Helmholtz Association.

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