2020
DOI: 10.1016/j.colsurfa.2020.125075
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Reducing the droplet/solid interfacial sliding resistance under electrowetting-on-dielectric by different voltage slew rate signals

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Cited by 5 publications
(5 citation statements)
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“…where C D , A D , ρ f and U denote the drag coefficient, projected area, air density and droplet velocity, respectively. [13] According to the observation of Oprins et al, [22] it is found that when air is the filling medium the resistance can be ignored. The imbalance of electric field force and friction force will cause acceleration on the contact line.…”
Section: Dynamic Contact Angle Modelmentioning
confidence: 99%
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“…where C D , A D , ρ f and U denote the drag coefficient, projected area, air density and droplet velocity, respectively. [13] According to the observation of Oprins et al, [22] it is found that when air is the filling medium the resistance can be ignored. The imbalance of electric field force and friction force will cause acceleration on the contact line.…”
Section: Dynamic Contact Angle Modelmentioning
confidence: 99%
“…The amplitude and frequency of the droplet oscillation change differently with the surface wettability in different phase regimes. Ko et al [13] observed hydrodynamic flow in droplets using an AC voltage from a configuration with air as the ambient phase. The flow was observed using a laser sheet and fluorescent tracers, and a toroidal vortex flow was reported.…”
Section: Introductionmentioning
confidence: 99%
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“…One common way is to prestretch the droplet on the substrate using traditional EW. By suddenly releasing the electric voltage, the droplet recoils on the solid surface. , Dewetting is induced by the stored energy in the prestretched surface while in the whole process, the droplet is in contact with the inserted needle electrode. Recently, Edwards et al considered the dielectrowetting effect and induced droplet dewetting in a noncontactable manner, that is, by embedding a linear stripe array of interdigitated electrodes in the glass substrate.…”
Section: Introductionmentioning
confidence: 99%
“…Once dewetting completely, the droplet will detach from the hostile surface. In EW, droplet detachment was induced generally by the passive method as mentioned above, for example, by prestretching the interface and releasing the droplet to recoil and jump. However, the operating condition is quite strict. Experiments showed that a variety of factors influence the EW-induced detachment, such as external voltage, fluid viscosity, surface wettability, droplet volume, and so forth. ,, Vo and Tran investigated the critical conditions for jumping droplets in EW and established a criterion equation by taking account of contact line dissipation, pinning effect, droplet elasticity, and surface energy.…”
Section: Introductionmentioning
confidence: 99%