2021
DOI: 10.1021/acs.langmuir.1c01245
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Lubricant-Mediated Strong Droplet Adhesion on Lubricant-Impregnated Surfaces

Abstract: Lubricant-impregnated surfaces have recently emerged as a new type of multifunctional coating with a promising capability in exhibiting low friction or contact angle hysteresis. However, lubricant-infused surfaces severely suffer from the tensile droplet−lubricant adhesion. In this study, we show that lubricantinfused surfaces allow for a strong tensile droplet adhesion, which results in the generation of an offspring residual droplet when a droplet detaches from the surface. Such tensile liquid−liquid adhesio… Show more

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Cited by 9 publications
(11 citation statements)
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“…The droplet bouncing on nonwetting solid surfaces is ubiquitous in nature [16,17] and is important in many industrial processes like spraying, [18] anti-icing, [19][20][21] or self-cleaning. [22] There are three elementary parameters to characterize wetting properties of the solid surface (Figure 2): i) the contact angle θ of the droplet on the solid surface, [23][24][25][26] showing the static wetting property; ii) the contact angle hysteresis CAH = θ advancing -θ receding when droplet moves on the solid surface, [27][28][29][30] being the difference between the advancing angle θ advancing and receding angle θ receding and reflecting the mobility of the droplet on the solid surface; and iii) the sliding angle θ sliding , being the inclined angle of the solid surface when the droplet starts sliding. For droplet bouncing, the nonwetting solid surface typically should possess a high contact angle, a low contact angle hysteresis and a low sliding angle.…”
Section: Introductionmentioning
confidence: 99%
“…The droplet bouncing on nonwetting solid surfaces is ubiquitous in nature [16,17] and is important in many industrial processes like spraying, [18] anti-icing, [19][20][21] or self-cleaning. [22] There are three elementary parameters to characterize wetting properties of the solid surface (Figure 2): i) the contact angle θ of the droplet on the solid surface, [23][24][25][26] showing the static wetting property; ii) the contact angle hysteresis CAH = θ advancing -θ receding when droplet moves on the solid surface, [27][28][29][30] being the difference between the advancing angle θ advancing and receding angle θ receding and reflecting the mobility of the droplet on the solid surface; and iii) the sliding angle θ sliding , being the inclined angle of the solid surface when the droplet starts sliding. For droplet bouncing, the nonwetting solid surface typically should possess a high contact angle, a low contact angle hysteresis and a low sliding angle.…”
Section: Introductionmentioning
confidence: 99%
“…[ 27 ] To explain the divergent spring behaviors for different‐sized patterns, we investigate the origin of the tensile force generated by the droplet‐based spring. The tensile force is the sum of the Laplace pressure F L (related to the droplet‐solid contact area and the contact angle) and the surface tension F S (related to the length of the TCL and the contact angle), [ 28 ] and the latter is dominant. For small patterns, with the stretching of the spring, the contact angle of the droplet gradually decreases and approaches 90° before break‐up of the liquid bridge, which maintains the increasing trend of the surface tension.…”
Section: Resultsmentioning
confidence: 99%
“…It shows a constant depletion speed of 1.4 nL/drop ±0.3 nL/drop. As schematically shown in Figure b, an annular wetting ridge and a cloaking layer are always formed when water drops slide on the lubricant-infused surfaces. ,, Therefore, the lubricant-depletion may be caused by the cloaking layer and meniscus.…”
Section: Resultsmentioning
confidence: 99%