2012
DOI: 10.1103/physrevlett.109.116101
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Evaporation of Droplets on Superhydrophobic Surfaces: Surface Roughness and Small Droplet Size Effects

Abstract: Evaporation of a sessile droplet is a complex, nonequilibrium phenomenon. Although evaporating droplets upon superhydrophobic surfaces have been known to exhibit distinctive evaporation modes such as a constant contact line (CCL), a constant contact angle (CCA), or both, our fundamental understanding of the effects of surface roughness on the wetting transition remains elusive. We show that the onset time for the CCL-CCA transition and the critical base size at the Cassie-Wenzel transition exhibit remarkable d… Show more

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Cited by 200 publications
(210 citation statements)
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“…Micro-nano hierarchical textures have been proved to be able to effectively prevent the C-W transition by experiments 16,22,[28][29][30]39,40 . But detailed theoretical analysis is very limited.…”
Section: Effects Of Micro-nano Hierarchical Textures On C-w Transitiomentioning
confidence: 99%
“…Micro-nano hierarchical textures have been proved to be able to effectively prevent the C-W transition by experiments 16,22,[28][29][30]39,40 . But detailed theoretical analysis is very limited.…”
Section: Effects Of Micro-nano Hierarchical Textures On C-w Transitiomentioning
confidence: 99%
“…Compared with surfaces with single-scale roughness, higher free energy and higher ACA for given ˛1 and x 1 are obtained in surfaces with dual-scale roughness, particularly those with structured sidewalls. External pressures, such as the vibrations and evaporation of a droplet [44,45], are required for a system at rest to start moving toward higher free energy states. The normalized minimum free energy (G * min ) CB-CB→CB-W for the transition from the CB-CB state to the CB-W state consists of two parts.…”
Section: Wetting Transition and Superhydrophobic Stabilitymentioning
confidence: 99%
“…When water droplet evaporates in the CCR mode, attributing to contact angle hysteresis (CAH) [11] (Fig. 1a) which is mainly associated with line tension [12,13], there is a pinning force per unit length acting at the three-phase contact line in the lateral direction f pin = γ lv (cos θ r − cos θ a ),…”
Section: Introductionmentioning
confidence: 99%