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Abstract
The time courses of the nanobubbles were investigated on a highly oriented pyrolytic graphite (HOPG) surface contacting with the air-saturated water-ethanol mixture. On a high step density surface, bubbles were confined within a narrow bunched terrace, and coalesced to form an elliptic bubble. The final volume of the coalesced bubble was larger than that of the sum of the initial individual bubbles. On a ider terrace, the volume of a solitary hemispherical bubble changed stochastically and the larger volume fluctuation accompanied a smaller bubble.
The time courses of the nanobubbles were investigated on a highly oriented pyrolytic graphite (HOPG) surface contacting with the air-saturated water–ethanol mixture. On a high step density surface, bubbles were confined within a narrow bunched terrace, and coalesced to form an elliptic bubble. The final volume of the coalesced bubble was larger than that of the sum of the initial individual bubbles. On a wider terrace, the volume of a solitary hemispherical bubble changed stochastically and the larger volume fluctuation accompanied a smaller bubble.
Journal
- Jpn J Appl Phys
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Jpn J Appl Phys 47(2), 1065-1067, 2008-02-25
INSTITUTE OF PURE AND APPLIED PHYSICS
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