The Young–Laplace equation suggests that nanosized
gas clusters
would dissolve under the effects of perturbation. The fact that nanobubbles
are observed raises questions as to the mechanism underlying their
stability. In the current study, we used all-atom molecular dynamics
simulations to investigate the gas–water interfacial properties
of gas clusters. We employed the instantaneous coarse-graining method
to define the fluctuating boundaries and analyze the deformation of
gas clusters. Fourier transform analysis of the cluster morphology
revealed that the radius and morphology deformation variations exhibit
power law relationships with the vibrational frequency, indicating
that the surface energy dissipated through morphology variations.
Increasing pressure in the liquid region was found to alter the network
of water molecules at the interface, whereas increasing pressure in
the gas region did not exhibit this effect. The overall gas concentration
was oversaturated and proportional to the gas density inside the clusters.
However, the result of comparison with Henry’s law reveals
that the gas pressure at the interface reduced by the interfacial
effects is much lower than that inside the gas region, thus reducing
the demanding degree of oversaturation. Originating from the interfacial
charge allocation, the magnitude of the electrostatic stress is greater
than that of the gas pressure inside the cluster. However, the magnitude
of the reversed tension induced by electrostatic stress is far below
the value of interfacial tension. The potential of mean force (PMF)
profiles revealed that a barrier potential at the interface hindered
gas particles from escaping the cluster. Several effects contribute
to stabilizing the gas clusters in water, including high-frequency
morphological deformation, electrostatic stress, reduced interfacial
tension, and gas oversaturation conditions. Our results suggest that
gas clusters can exist in water under gas oversaturation conditions
in the absence of hydrophobic contaminants or pinning charges at interfaces.