1990
DOI: 10.1017/s0022112090002336
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Buoyancy-driven motion of a deformable drop toward a planar wall at low Reynolds number

Abstract: The slow viscous motion of a deformable drop moving normal to a planar wall is studied numerically. In particular, a boundary integral technique employing the Green's function appropriate to a no-slip planar wall is used. Beginning with spherical drop shapes far from the wall, highly deformed and 'dimpled ' drop configurations are obtained as the planar wall is approached. The initial stages of dimpling and their evolution provide information and insight into the basic assumptions of filmdrainage theory.

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Cited by 44 publications
(19 citation statements)
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“…For example, in the case of flow in an infinite domain, p j (x, x 0 ) = 2x j /|x| 3 . The second integral on the right-hand side of (3.10) is the double-layer potential with vectorial strength proportional to the normal vector.…”
Section: Double-layer Representationmentioning
confidence: 99%
“…For example, in the case of flow in an infinite domain, p j (x, x 0 ) = 2x j /|x| 3 . The second integral on the right-hand side of (3.10) is the double-layer potential with vectorial strength proportional to the normal vector.…”
Section: Double-layer Representationmentioning
confidence: 99%
“…Subsequently, Tsurutani et al [7] enhanced the MAC model to include surface tension and viscosity effects, improving considerably the accuracy of the simulations. Since then, numerous papers have been published reporting two-dimensional and three-dimensional [8][9][10] droplet impact simulations and the introduction of more refined numerical techniques to improve predictions, including the use of adaptative grids [11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…This transient effect will clearly have little effect on the removal of sub-retinal fluid. As the bubble floats upward toward the retina, its behavior can be described by numerical simulations of the governing fluid-dynamic equations [8], as performed by Manga and Stone [9] and Ascoli et al [2]. If the bubble is large and envelopes the entire tear, its buoyancy force will be directed upwards on the RPE peripheral to the flap, rather than on the flap itself.…”
Section: Discussionmentioning
confidence: 99%