Self-excited potential oscillation of lipid across a micropore controlled by hydrostatic pressure

Seimei Shiratori, Takamichi Nakamoto, Toyosaka Moriizumi

研究成果: Article

1 引用 (Scopus)

抄録

Effects of the hydrostatic pressure difference across the oil to water interface on a self-excited potential oscillation at a micropore have been investigated by potential measurement and microscopic observation. The amplitude and frequency of the oscillation are precisely controlled by means of changing the hydrostatic pressure. This effect of hydrostatic pressure is due to the change in the diameter of a dome that is built at the micropore. These results are qualitatively consistent with our previous ones [Jpn. J. Appl. Phys. 30 (1991) L1435]; i.e., the self-excited potential oscillation can be controlled through changes in the shape or the size of the interface.

元の言語English
ジャーナルJapanese Journal of Applied Physics, Part 2: Letters
32
発行部数1 A-B
出版物ステータスPublished - 1993
外部発表Yes

Fingerprint

Hydrostatic pressure
hydrostatic pressure
Lipids
lipids
oscillations
Domes
domes
oils
water
Water

ASJC Scopus subject areas

  • Physics and Astronomy (miscellaneous)

これを引用

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N2 - Effects of the hydrostatic pressure difference across the oil to water interface on a self-excited potential oscillation at a micropore have been investigated by potential measurement and microscopic observation. The amplitude and frequency of the oscillation are precisely controlled by means of changing the hydrostatic pressure. This effect of hydrostatic pressure is due to the change in the diameter of a dome that is built at the micropore. These results are qualitatively consistent with our previous ones [Jpn. J. Appl. Phys. 30 (1991) L1435]; i.e., the self-excited potential oscillation can be controlled through changes in the shape or the size of the interface.

AB - Effects of the hydrostatic pressure difference across the oil to water interface on a self-excited potential oscillation at a micropore have been investigated by potential measurement and microscopic observation. The amplitude and frequency of the oscillation are precisely controlled by means of changing the hydrostatic pressure. This effect of hydrostatic pressure is due to the change in the diameter of a dome that is built at the micropore. These results are qualitatively consistent with our previous ones [Jpn. J. Appl. Phys. 30 (1991) L1435]; i.e., the self-excited potential oscillation can be controlled through changes in the shape or the size of the interface.

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