2008
DOI: 10.1088/0034-4885/71/3/036601
|View full text |Cite
|
Sign up to set email alerts
|

Physics of liquid jets

Abstract: Jets, i.e. collimated streams of matter, occur from the microscale up to the large-scale structure of the universe. Our focus will be mostly on surface tension effects, which result from the cohesive properties of liquids. Paradoxically, cohesive forces promote the breakup of jets, widely encountered in nature, technology and basic science, for example in nuclear fission, DNA sampling, medical diagnostics, sprays, agricultural irrigation and jet engine technology. Liquid jets thus serve as a paradigm for free-… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

40
1,118
3
17

Year Published

2010
2010
2021
2021

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 1,552 publications
(1,247 citation statements)
references
References 539 publications
40
1,118
3
17
Order By: Relevance
“…The experiments show that breakup lengths increase with injection velocity for small injection velocities and then reduce for larger velocities before eventually levelling off (see figure 13 of Hiroyasu et al 1982 which is reproduced as figure 1 here). In the comprehensive review paper by Eggers & Villermaux (2008) the reducing breakup length for larger velocities is explained by the thinning shear velocity at the edge of the jet, but no explanation is given for the rise in the breakup length for small velocities. In this paper we show that the increasing breakup length for small velocities could be due to the value of the fluid velocity at the fluid interface within the shear layer increasing with velocity.…”
Section: Introductionmentioning
confidence: 99%
“…The experiments show that breakup lengths increase with injection velocity for small injection velocities and then reduce for larger velocities before eventually levelling off (see figure 13 of Hiroyasu et al 1982 which is reproduced as figure 1 here). In the comprehensive review paper by Eggers & Villermaux (2008) the reducing breakup length for larger velocities is explained by the thinning shear velocity at the edge of the jet, but no explanation is given for the rise in the breakup length for small velocities. In this paper we show that the increasing breakup length for small velocities could be due to the value of the fluid velocity at the fluid interface within the shear layer increasing with velocity.…”
Section: Introductionmentioning
confidence: 99%
“…The Ohnesorge number is the ratio of the viscous capillary timescale to the capillary timescale. We describe the liquid jet by the one-dimensional model (Trouton 1906;Weber 1931;Eggers & Villermaux 2008)…”
Section: Base Flowmentioning
confidence: 99%
“…Capillary breakup occurs within a time τ which depends on the thread radius h, on the liquid density ρ, viscosity η and surface tension γ, and we know that most of this time is spent at developing an instability about the quasi-columnar shape of the thread, the subsequent phenomena occurring around the pinching instant at the drops separation being comparatively much faster (Eggers & Villermaux 2008). The time τ is either the capillary time ρh 3 /γ when inertia and surface tension are solely at play, or the viscous capillary time ηh/γ if viscous effects dominantly slow down the unstable dynamics.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Surface tension affects the drop formation process, the breakup of jets [23] and the oscillations of the shapes of drops. Surface tension tends to keep the drops spherical in flight since spherical shapes minimize the surface energy [24].…”
Section: Fluid Dynamics Descriptionmentioning
confidence: 99%