2001
DOI: 10.1017/s0022112000003268
|View full text |Cite
|
Sign up to set email alerts
|

Viscous beads on vertical fibre

Abstract: The dynamics of a thick layer of viscous liquid flowing down a thin vertical fibre is investigated. Three qualitatively different regimes of the interfacial patterns in the form of beads were observed experimentally. Two typical regimes at relatively small flow rate are described reasonably well by the creeping-flow model equation proposed here.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

20
223
2

Year Published

2012
2012
2024
2024

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 151 publications
(257 citation statements)
references
References 18 publications
20
223
2
Order By: Relevance
“…1 in Ref. [8]. In the first case of flow regime (a), the drops are large and move rapidly and the flow rates are relatively large.…”
Section: Introductionmentioning
confidence: 94%
See 1 more Smart Citation
“…1 in Ref. [8]. In the first case of flow regime (a), the drops are large and move rapidly and the flow rates are relatively large.…”
Section: Introductionmentioning
confidence: 94%
“…Kliakhandler et al [8] conducted experiments that revealed the richness of the dynamics of the flow of a thick film down a vertical fiber. Three qualitatively different regimes of the interfacial patterns in the form of beads were observed experimentally.…”
Section: Introductionmentioning
confidence: 99%
“…Kliakhandler, Davis, and Bankoff [12] conducted experiments that revealed the richness of the dynamics of the flow * rongliu@guet.edu.cn † z.ding@bristol.ac.uk down a vertical fiber. In their experiments, the film is at least twice as thick as the fiber radius.…”
Section: Introductionmentioning
confidence: 99%
“…The authors proposed an evolution equation that does not rely on the previously made thin-film assumptions. Craster and Matar [13] derived a new evolution equation similar to that used by Kliakhandler, Davis, and Bankoff [12], and they revisited the same problem in which the fluid radius is much smaller than its characteristic length based upon a capillary length scale.…”
Section: Introductionmentioning
confidence: 99%
“…We utilise their experimental parameters for silicon oil here; they are γ = 21.9 dyn/cm, ρ = 0.986 g/cm 3 , and H = 0.085 cm. Equation (1) was derived under the assumption that H L to ensure the thinness of the film, but also requires that H R. The complementary regime of flow down the outside of a narrow fibre, for which the radius of the cylinder is much less than the film thickness, was investigated in many previous studies [3,6].…”
Section: C379mentioning
confidence: 99%