2013
DOI: 10.1063/1.4805068
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The fastest drop climbing on a wet conical fibre

Abstract: We use high-speed video imaging to study the capillary-driven motion of a micro-droplet along the outside of a pre-wetted conical fiber. The cones are fabricated on a glass-puller with tip diameters as small as 1 μm, an order of magnitude smaller than in previous studies. The liquid is fed through the hollow fiber accumulating at the fiber tip to form droplets. The droplets are initially attached to the opening as they grow in size before detaching and traveling up the cone. This detachment can produce a trans… Show more

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Cited by 23 publications
(17 citation statements)
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References 22 publications
(18 reference statements)
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“…2D and Fig. S2), and thus an asymmetric surface energy landscape, which permits a motion (12)(13)(14)(15). A simple argument allows us to understand the origin of the driving force.…”
mentioning
confidence: 99%
“…2D and Fig. S2), and thus an asymmetric surface energy landscape, which permits a motion (12)(13)(14)(15). A simple argument allows us to understand the origin of the driving force.…”
mentioning
confidence: 99%
“…Most of the previous studies consider the motion of axisymmetrical barrel shape droplets moving on conical substrates. The models are based on a driving force coming from a gradient of the Laplace pressure along the surface of the droplet [19,22]. In our case, the barrel shape is not axisymmetrical due to gravitational effects.…”
Section: A Barrel Shapementioning
confidence: 99%
“…Those cones were created by pulling a cylindrical copper wire out of an acid bath. Other studies used different ways to manufacture conical fibers like pulling glass [22][23][24][25], using an electrochemical corrosion gradient [26] or even polishing brass [27]. According to the relative size of the fiber and of the droplet, the droplet on cylindrical and conical fibers can present two distinct geometries: barrel or clamshell [28].…”
Section: Introductionmentioning
confidence: 99%
“…Common to fluid coating processes is that they often require an external driving force to displace the fluid. However, when a droplet with a size smaller than the capillary length comes in contact with a conical fibre, it moves spontaneously from the tip to the base of the cone due to capillarity (Lorenceau & Quéré 2004;Li & Thoroddsen 2013). In nature, this self-propelled mechanism has been exploited by plants (Liu et al 2015) and animals (Zheng et al 2010;Wang et al 2015) to facilitate water transport at small scales.…”
Section: Introductionmentioning
confidence: 99%