Abstract
Nanobubble formation and binding to nanoelectrodes significantly hinder the efficiency of gas evolution reactions, limiting the potential of hydrogen production technologies. This work uncovers the pivotal role of nanoelectrode shape in influencing catalytic performance and nanobubble detachment. Using molecular dynamics simulations supported by experimental evidence, we establish that nanoparticle electrodes with convex geometries (e.g. hemispheres, spheres, cubes) sustain higher catalytic performance by maintaining greater reactive surface exposure than flat or concave electrodes. Most importantly, we demonstrate that convex nanoparticle electrodes mitigate bubble pinning by promoting unlimited growth and spontaneous detachment. We develop a diffusional theory that explains and generalizes our simulations, predicting the onset currents that drive nanobubbles into a non-stationary growth regime. This theory reveals that the transition to continuous bubble growth occurs when the electrochemically generated gas rate surpasses the diffusion-limited escape rate, independent of electrode size and convex shape but sensitive to the electrode support. The theoretical model extends the predictions to other gas-evolving electrochemical processes, highlighting its relevance for diverse catalytic systems. Surprisingly, our calculations reveal that bubble detachment contributes minimally to the total current. Instead, the enhanced catalytic efficiency of convex electrodes stems from their ability to sustain an exposed reactive surface, even during bubble growth. These findings provide a fundamental framework for designing nanoelectrodes that optimize gas evolution by prioritizing surface exposure rather than relying solely on bubble detachment.
Supplementary materials
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Supporting Methods and Supporting Results
Description
force field (Section A.1); parameterization (Section A.2); modeling of the reaction kinetics at constant potential (Section A.3); calibration of Butler-Volmer kinetics (Section A.4); derivation of the critical current equations and calculation of critical currents (Section A.5); exposed area of the electrode (Section B.1); size of bubble and current (Section B.2); exposed area vs potential (Section B.3); nanobubble formation on cubic nanoparticle (Section B.4); lifetime of lifted growing bubble on 7 nm2 hemispherical electrode(Section B.5); lifetime of the lifted growing bubble on 14 nm2 spherical electrode (Section B.6); predictions on the lifetime of bound and lifted growing bubble on sphere electrode with 70 nm diameter in experiments (Section B.7); tables of lifetime of bound and lifted growing bubble at the critical potential (Section B.8); contribution of nucleation process from nucleation-growth-detachment cycle for the bubble (Section B.9); predictions of the threshold current in our simulations (Section B.10) (PDF)
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Movie 1
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Side view of nanobubble evolution from bound to lifted state on a 7 nm2 hemispherical electrode at 632 mV
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Movie 2
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Side view of nanobubble evolution from bound to lifted state on a 14 nm2 spherical electrode at 557 mV
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Movie 3
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Side view of lifted nanobubble on a 14 nm2 floating spherical electrode at 557 mV
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