Journal
MOLECULES
Volume 26, Issue 21, Pages -Publisher
MDPI
DOI: 10.3390/molecules26216719
Keywords
air-water interface; Hofmeister series; hydrogen bonding; charge transfer; symmetry-adapted perturbation theory; noncovalent interactions
Funding
- U.S. National Science Foundation [CHE-1955282]
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Soft anions exhibit surface activity at the air/water interface, with some showing larger charge-transfer energy at the interface compared to bulk water. However, the contribution of these effects to the surface activity of soft anions is small and cannot fully explain the observed behavior. The short-range solvation structure around these ions at the air/water interface is scarcely different from bulk water, suggesting that changes in hydration structure may not be the key factor in soft anions' surface activity.
Soft anions exhibit surface activity at the air/water interface that can be probed using surface-sensitive vibrational spectroscopy, but the structural implications of this surface activity remain a matter of debate. Here, we examine the nature of anion-water interactions at the air/water interface using a combination of molecular dynamics simulations and quantum-mechanical energy decomposition analysis based on symmetry-adapted perturbation theory. Results are presented for a set of monovalent anions, including Cl-, Br-, I-, CN-, OCN-, SCN-, NO2-, NO3-, and ClOn- (n=1,2,3,4), several of which are archetypal examples of surface-active species. In all cases, we find that average anion-water interaction energies are systematically larger in bulk water although the difference (with respect to the same quantity computed in the interfacial environment) is well within the magnitude of the instantaneous fluctuations. Specifically for the surface-active species Br-(aq), I-(aq), ClO4-(aq), and SCN-(aq), and also for ClO-(aq), the charge-transfer (CT) energy is found to be larger at the interface than it is in bulk water, by an amount that is greater than the standard deviation of the fluctuations. The Cl-(aq) ion has a slightly larger CT energy at the interface, but NO3-(aq) does not; these two species are borderline cases where consensus is lacking regarding their surface activity. However, CT stabilization amounts to < 20% of the total induction energy for each of the ions considered here, and CT-free polarization energies are systematically larger in bulk water in all cases. As such, the role of these effects in the surface activity of soft anions remains unclear. This analysis complements our recent work suggesting that the short-range solvation structure around these ions is scarcely different at the air/water interface from what it is in bulk water. Together, these observations suggest that changes in first-shell hydration structure around soft anions cannot explain observed surface activities.
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