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The boundary layer on a spherical gas bubble

Moore, D. W.·1963·Journal of Fluid Mechanics

Abstract

The equations governing the boundary layer on a spherical gas bubble rising steadily through liquid of small viscosity are derived. These equations are linear are linear and are solved in closed form. The boundary layer separates at the rear stagnation point of the bubble to form a thin wake, whose structure is determined. Thus the drag force can be calculated from the momentum defect. The value obtained is 12πa aU μ, where a is the bubble radius and U the terminal velocity, and this agrees with the result of Levich (1949) who argued from the viscous dissipation in the potential flow round the bubble. The next term in an expansion of the drag in descending fractional powers of R is found and the results compared with experiment.

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Metadata

Authors
Moore, D. W.
Venue
Journal of Fluid Mechanics
Published
1963-06
Volume
16
Issue
2
Pages
161-176
ISSN
  • 0022-1120 (ISSN-L)
  • 1469-7645
OpenAlex
W2040790971
Cited by
510
References
0
FWCI
8.09
Type
journal article
Language
en
Open access
closed

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CoChat. (2026). Citation check: The boundary layer on a spherical gas bubble. https://app.cochat.ai/papers/10.1017/s0022112063000665
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Moore, D. W. (1963). The boundary layer on a spherical gas bubble. Journal of Fluid Mechanics. https://doi.org/10.1017/s0022112063000665

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Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).

Semantic Scholar’s data is described in: Kinney, R., et al. (2023). The Semantic Scholar Open Data Platform. arXiv:2301.10140.