2021
DOI: 10.1140/epje/s10189-021-00014-z
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Droplet migration on conical fibers

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Cited by 5 publications
(17 citation statements)
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“…For droplets below the capillary length, motion is driven by the surface tension of the droplet to maximize contact with the fiber when the droplet wets the fiber. 11,[17][18][19][20] As the characteristic size of the droplet becomes larger than the capillary length, the droplet may either be propelled [21][22][23][24] or stalled 25 by gravity depending on the fiber orientation. Droplet motion can also be induced in these systems by temperature gradients or coatings.…”
Section: Introductionmentioning
confidence: 99%
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“…For droplets below the capillary length, motion is driven by the surface tension of the droplet to maximize contact with the fiber when the droplet wets the fiber. 11,[17][18][19][20] As the characteristic size of the droplet becomes larger than the capillary length, the droplet may either be propelled [21][22][23][24] or stalled 25 by gravity depending on the fiber orientation. Droplet motion can also be induced in these systems by temperature gradients or coatings.…”
Section: Introductionmentioning
confidence: 99%
“…26,27 The motion of a single droplet on a slender conical structure has been studied and characterized extensively, with an excellent understanding of the driving forces and viscous dissipation in the droplet. 17,19,20,23,[28][29][30][31] Furthermore, previous works have examined the formation of multiple droplets via the Plateau-Rayleigh instability (PRI) of a film of liquid on a cylindrical fiber. 32,33 In addition, studies have examined wetting and coalescence of droplets on a fiber network with particular interest in droplet capture in textiles [34][35][36][37][38] However, there has been little work on the formation and interaction between multiple droplets as they traverse along a conical fiber beyond qualitative observations, 17,32,39 despite being prevalent in nature as illustrated in Fig.…”
Section: Introductionmentioning
confidence: 99%
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