Abstract
The surface of an air bubble is a particularly simple one at which to examine the electrical conditions which attend all small particles when immersed in a liquid. An air bubble may be considered as a type of coarse suspensoid, which, on being immersed in water, acquires a charge and moves in an electric field as if negatively electrified. The present work is a continuation of that already published ('Roy. Soc. Proc.,' A, vol. 106, p. 315 (1924)) and deals chiefly with the charge on the bubble immediately after it enters the liquid; this is examined experimentally and also theoretically. In addition, a new method of calculating the potential difference between the bubble surface and the interior of the liquid is suggested.
Dates
Type | When |
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Created | 18 years, 8 months ago (Dec. 18, 2006, 4:30 p.m.) |
Deposited | 4 years, 6 months ago (Feb. 21, 2021, 12:21 a.m.) |
Indexed | 1 year, 4 months ago (April 22, 2024, 9:51 a.m.) |
Issued | 99 years, 1 month ago (Aug. 3, 1926) |
Published | 99 years, 1 month ago (Aug. 3, 1926) |
Published Online | 28 years, 8 months ago (Jan. 1, 1997) |
Published Print | 99 years, 1 month ago (Aug. 3, 1926) |
@article{1926, volume={112}, ISSN={2053-9150}, url={http://dx.doi.org/10.1098/rspa.1926.0108}, DOI={10.1098/rspa.1926.0108}, number={760}, journal={Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character}, publisher={The Royal Society}, year={1926}, month=aug, pages={235–251} }