Pancake bouncing of impacting nanodroplets on smooth and nanopillared surfaces

被引:1
|
作者
Ma, Qiang [1 ,2 ,3 ,4 ]
Wang, Yi-Feng [1 ,2 ]
Wu, Chuan-Wei [3 ]
Yang, Yan-Ru [1 ,2 ]
Zheng, Shao-Fei [1 ,2 ]
Tran, Tuan [3 ]
Wang, Xiao-Dong [1 ,2 ]
机构
[1] North China Elect Power Univ, State Key Lab Alternate Elect Power Syst Renewable, Beijing 102206, Peoples R China
[2] North China Elect Power Univ, Res Ctr Engn Thermophys, Beijing 102206, Peoples R China
[3] Nanyang Technol Univ, Sch Mech & Aerosp Engn, 50 Nanyang Ave, Singapore 639798, Singapore
[4] Ordos Vocat Coll, Dept Architectural Engn, Ordos 017000, Peoples R China
基金
中国国家自然科学基金;
关键词
Pancake bouncing; Nanodroplet; Contact time; Molecular dynamics; CONTACT TIME; DROP IMPACT; LIQUID-DROP; DYNAMICS; BEHAVIOR; MODEL;
D O I
10.1016/j.icheatmasstransfer.2024.108108
中图分类号
O414.1 [热力学];
学科分类号
摘要
Reducing the contact time of impacting droplets on solid surfaces has become a research focus due to its promising application prospects in self-cleaning, anti-erosion, and anti-icing. In this study, the pancake bouncing of nanodroplets is investigated through molecular dynamics simulations, achieving a remarkable reduction in contact time. Two distinct patterns of pancake bouncing are identified when nanodroplets impact smooth and nanopillared surfaces with different bouncing mechanisms. The first pancake bouncing pattern with holes on smooth surfaces is attributed to internal-flow collision induced by multiple retraction centers. The second pancake bouncing pattern on nanopillared surfaces results from the storage and release of sufficient surface energy due to liquid penetration and requires satisfying both the timescale and energy criterion. Subsequently, theoretical models for two criteria are developed, which promote two parameter groups (-(s(2) + 2ws)h(wcos theta(0))(-1) and We(-1/3)Re(-1/3)R(0)(2)) corresponding to the surface and droplet. Based on these two parameter groups, a phase diagram is established and indicates the triggering conditions for the second pancake bouncing patterns. Finally, it is further revealed that by increasing the pillar height from smooth to nanopillared surfaces, the bouncing regime is transformed from the first pancake bouncing pattern, regular bouncing, to the second pancake bouncing pattern.
引用
收藏
页数:12
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