2019
DOI: 10.1016/j.ces.2019.02.041
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Asymmetric coalescence-induced droplet jumping on hydrophobic fibers

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Cited by 5 publications
(5 citation statements)
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“…Comparing Figure with Figure a, it can be found that in C 7 H 8 , the morphology evolution and the overall coalescence time of the merged droplets were similar to those in n -C 6 H 14 , but the number of coalescence stages was only four stages, and the coalescence time of each stage was longer than that in n -C 6 H 14 . It is well known that the driving force for the droplet morphology and droplet jumping is excess surface energy, which is proportional to the oil–water interfacial tension. , As shown in Table , the oil–water interfacial tension of C 7 H 8 is 35.7 mN/m, which is only about 70.7% that of n -C 6 H 14 . Hence, the frequency of droplet morphology evolution in C 7 H 8 was lower than that in n -C 6 H 14 , i.e., the time required for each stage of droplet deformation was larger than that in n -C 6 H 14 , as shown in Figure .…”
Section: Resultsmentioning
confidence: 99%
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“…Comparing Figure with Figure a, it can be found that in C 7 H 8 , the morphology evolution and the overall coalescence time of the merged droplets were similar to those in n -C 6 H 14 , but the number of coalescence stages was only four stages, and the coalescence time of each stage was longer than that in n -C 6 H 14 . It is well known that the driving force for the droplet morphology and droplet jumping is excess surface energy, which is proportional to the oil–water interfacial tension. , As shown in Table , the oil–water interfacial tension of C 7 H 8 is 35.7 mN/m, which is only about 70.7% that of n -C 6 H 14 . Hence, the frequency of droplet morphology evolution in C 7 H 8 was lower than that in n -C 6 H 14 , i.e., the time required for each stage of droplet deformation was larger than that in n -C 6 H 14 , as shown in Figure .…”
Section: Resultsmentioning
confidence: 99%
“…It is well known that the driving force for the droplet morphology and droplet jumping is excess surface energy, which is proportional to the oil−water interfacial tension. 27,28 As shown in Table 1, the oil−water interfacial tension of C 7 H 8 is 35.7 mN/m, which is only about 70.7% that of n-C 6 H 14 . Hence, the frequency of droplet morphology evolution in C 7 H 8 was lower than that in n-C 6 H 14 , i.e., the time required for each stage of droplet deformation was larger than that in n-C 6 H 14 , as shown in Figure 6.…”
Section: Effect Of Bulk Fluid Viscositymentioning
confidence: 99%
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“…Droplet coalescence jumping could facilitate droplets to leave superhydrophobic surfaces spontaneously, which has extensive prospects in self-cleaning, energy harvesting, atmospheric corrosion protection, , and anti-icing/frosting. , In those applications, the jumping direction and velocity are important factors affecting the performance. The jumping velocity V j of the coalescence of two equal-sized droplets follows the capillary-inertial scaling. , Previous studies have demonstrated that size mismatch, quantity, and distribution have a negligible effect on jumping direction. , Nevertheless, the jumping velocity is less than that of when two equal-sized droplets coalesced. , …”
Section: Introductionmentioning
confidence: 93%
“…Nanodroplets have wide applications in various fields such as the self‐assembly of nanomaterials, fluid transport, catalysis, and 3D nanoinkjet printing . In these applications, coalescence is a significant process as it determines the formation and evolution of the droplet . Moreover, it has been widely observed and shown that the size distribution of droplets is dominated by coalescence .…”
Section: Introductionmentioning
confidence: 99%