2011
DOI: 10.1039/c1cp22018g
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Molecular dynamics study on helium nanobubbles in water

Abstract: Interfacial properties of helium nanobubbles in water at normal conditions have been investigated using large-scale molecular dynamics simulations for systems including over one million atoms. The surface tension of a helium nanobubble is a convex function with respect to the bubble radius, and is estimated to vanish at a critical radius of approximately 1 nm.

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Cited by 18 publications
(13 citation statements)
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“…28 Amber FF03 29 was used to model the interaction of the carbon of the pristine graphene (atom type CA), which has been shown previously to describe structure and dynamics of confined water very well. The same helium parameters were used recently 34 to study the stability of helium bubbles in water. During minimization, the pristine graphene sheets were held fixed to their initial positions using a harmonic constraint with a spring constant of 500 kcal mol À1 Å À2 .…”
Section: Simulation Detailsmentioning
confidence: 99%
“…28 Amber FF03 29 was used to model the interaction of the carbon of the pristine graphene (atom type CA), which has been shown previously to describe structure and dynamics of confined water very well. The same helium parameters were used recently 34 to study the stability of helium bubbles in water. During minimization, the pristine graphene sheets were held fixed to their initial positions using a harmonic constraint with a spring constant of 500 kcal mol À1 Å À2 .…”
Section: Simulation Detailsmentioning
confidence: 99%
“…16,17 Ashbaugh and Pratt 4 find δ ≈ 0.6 Å at T = 300 K, which decreases with increasing temperature and changes sign at T ≈ 350 K. Huang et al 18 deduce δ = 0.9 Å at T = 298 K for SPC/E water from simulated solvation free energies of hydrophobic spheres. Yamamoto and Ohnishi 19 on the other hand find a maximum in the surface tension of helium bubbles in water as a function of bubble radius, which, considering the curvature expansion in Eqs. (1) or (3), corresponds to a negative Tolman length, in contrast to the previous studies.…”
Section: Introductionmentioning
confidence: 96%
“…Here, d Using DFT, Talanquer et al [66] calculated the density profiles of unstable critical bubbles at R = R c , where the solute is accumulated in the bubble interior and its density exhibits a mild maximum at the interface. In their molecular dynamics simulation, Yamamoto and Ohnishi [67] realized stable helium-rich nanobubbles in water. They fixed the cell volume to find slightly negative pressures in the liquid region as in our Fig.6(a).…”
Section: Stress Tensor Around a Bubble And Laplace Lawmentioning
confidence: 99%