Our @J_A_C_S study (https://t.co/Y1OuKtjnO8) shows nanobubbles strongly prefer staying at the TiO₂–water interface. Detaching a ~3 nm N₂ nanobubble requires ~150 kJ/mol, making spontaneous release unlikely—highlighting why bubble removal often needs growth or external forces.
Our @J_A_C_S study (https://t.co/Y1OuKtjnO8) shows nanobubbles strongly prefer staying at the TiO₂–water interface. Detaching a ~3 nm N₂ nanobubble requires ~150 kJ/mol, making spontaneous release unlikely—highlighting why bubble removal often needs growth or external forces.
TiO₂ doesn’t always promote nucleation. The anatase (101) surface increases nucleation barriers, but in saline environments, the salting-out effect lowers the barrier—making TiO₂–NaCl systems most favorable for nanobubble formation.
🔥 The payoff: the rate-determining first N₂ hydrogenation drops to ~0.6 eV (ΔG ≈ 0.15 eV), finally matching experiments. Hydronium ions, H-bond networks, and local electric fields team up to make NRR easier than we thought.
🚀 Why does theory keep underestimating electrochemical N₂ reduction? Because water isn’t just a background. In our new work, we show that explicit solvent fundamentally rewires nitrogen reduction reaction at single-atom catalysts. Solvent ≠ spectator.
https://t.co/GOtvKpuJkr
💧 We used deep potential molecular dynamics with enhanced sampling to watch NRR happen in real water. No static snapshots, no implicit solvent—just long-time dynamics, proton shuttling, and a fully alive catalyst–electrolyte interface.
🚀 Based on Voronoi CV-based OPES DPLRMD, our new study reveals how electric fields & air-water interfaces switch glycine tautomerism mechanisms @JCIM_JCTC.
🔗 Article: https://t.co/qAqTyX7hRv
📂 Data: https://t.co/EG8GfOrOtW
#compchem#machinelearning#enhancedsampling
Background:
⚡️ Electric fields are EVERYWHERE in biology!
From enzyme electrostatics to membrane potentials → but how do they control amino acid proton transfer?
🔍 Glycine tautomerism = key model
💧 Solvent-driven PT pathways known
❓ UNKNOWN: Field/interface roles
🎬 The above trajectory is derived from the Voronoi CV-based OPES DPLRMD under a electric field of 10 mV/Å (Trajectory is translated as a whole with N as the box center)
🔑Color: H⚪ C⚫ N🔵 O🔴 Wannier centroid🟡
🔌 10 mV/Å field boosts [Z]→[N] by 10x via OH⁻-mediated path.
The follow-up work by @TrizioEnrico and @PeilinKang is out on @NatComputSci!🧨
A semi-automatic method to extensively sample "everywhere and everything" (metastable and transition states) "all at once" (in a single simulation) 🔥
📑: https://t.co/J8ScIuFo7W
Short🧵 @IITalk
@ACS_Langmuir At oil–water interfaces, hydronium ions are repelled into the bulk water, while hydroxide ions are enriched in the interfacial layer due to stabilization by positive charges from interfacial water and decane molecules.
Check out our latest preprint on double-layer distribution of hydronium and hydroxide ions at air/oil-water interfaces after water autoionization (https://t.co/U3UFugdkxO). #compchem#machinelearning#enhancedsampling (1/2)
@ACS_Langmuir This research investigates the behavior of hydronium and hydroxide ions at air/oil–water interfaces using enhanced-sampling molecular dynamics simulations with NNPs. The study finds that a stable ionic double-layer forms near the air–water interface. @ACS_Langmuir