2018
DOI: 10.1002/adfm.201800634
|View full text |Cite
|
Sign up to set email alerts
|

Bio‐Inspired Superhydrophobic Closely Packed Aligned Nanoneedle Architectures for Enhancing Condensation Heat Transfer

Abstract: Bionic condensate microdrop self‐propelling (CMDSP) surfaces are attracting intensive interest due to their academic and commercial values. Up to now, it is still a great challenge to design and fabricate CMDSP nanostructures with superior condensation heat transfer (CHT) efficiency. Here, it is reported that the CHT coefficient of copper surfaces can be enhanced maximally ≈320% via in situ growth and geometric regulation of closely packed aligned nanoneedles with CMDSP function. These experiments and theoreti… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
76
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
6
1

Relationship

0
7

Authors

Journals

citations
Cited by 71 publications
(79 citation statements)
references
References 37 publications
1
76
0
Order By: Relevance
“…Both the number and the distribution of combined droplets are important factors affecting the self-jumping speed [45,46] (Figure 3(c1-c3)). By adjusting the height, tip size and interspace of conical column structures (Figure 3(d1-d4)), Wang et al [47] obtained 320% enhancement on the condensation heat transfer coefficient compared with the smooth hydrophobic surface. [29], (a3) The sponge-like microfibrillar texture within the hair [29], (a4-a6) Hair deformation by water droplets [29]; (b1) The image of Cactus, (b2) SEM image of cactus spiny surface [32], (b3) The mechanism model of water droplet movement on cactus spiny surface [34], (b4) The image of superhydrophilic mastoids [38]; (c1) The image of Ruellia devosiana, (c2) The SEM image of Ruellia devosiana leaf [37], (c3) The image of the flat heat pipe with convex structure [39], (c4) Structure and working principle of the flat heat pipe with convex structure [39].…”
Section: Figure 2 (A1)mentioning
confidence: 99%
“…Both the number and the distribution of combined droplets are important factors affecting the self-jumping speed [45,46] (Figure 3(c1-c3)). By adjusting the height, tip size and interspace of conical column structures (Figure 3(d1-d4)), Wang et al [47] obtained 320% enhancement on the condensation heat transfer coefficient compared with the smooth hydrophobic surface. [29], (a3) The sponge-like microfibrillar texture within the hair [29], (a4-a6) Hair deformation by water droplets [29]; (b1) The image of Cactus, (b2) SEM image of cactus spiny surface [32], (b3) The mechanism model of water droplet movement on cactus spiny surface [34], (b4) The image of superhydrophilic mastoids [38]; (c1) The image of Ruellia devosiana, (c2) The SEM image of Ruellia devosiana leaf [37], (c3) The image of the flat heat pipe with convex structure [39], (c4) Structure and working principle of the flat heat pipe with convex structure [39].…”
Section: Figure 2 (A1)mentioning
confidence: 99%
“…In previous studies, [ 48,57 ] continuous self‐jumping behaviors were neglected although they were conducive to the departure of condensate dewdrops. As Figure 4d and Movie S1, Supporting Information, show, the continuous self‐jumping behaviors occur three times in a 210‐ms period.…”
Section: Resultsmentioning
confidence: 99%
“…The self‐jumping behaviors can be also negatively affected. In contrast, nanoarray/nanopore structures are favorable to self‐jumping, [ 48,49 ] owing to the excellent resistance to moisture penetration and dewdrop adhesion. [ 50,51 ] However, for water‐based coatings, considering only the nanostructure (nanopores) is inadequate and the microstructure (micropores) could have a serious effect on the repellency to condensate microdrops.…”
Section: Introductionmentioning
confidence: 99%
“…Superhydrophobic surfaces that have a water contact angle (WCA) greater than 150° and contact angle hysteresis (CAH) less than 10° have shown great promises for potential applications, including self‐cleaning, anti‐(bio)fouling, anti‐corrosion, anti‐icing and anti‐frosting, drag reduction, and enhanced heat transfer. [ 1–6 ] The non‐wettability and large water droplet mobility are attributed to hydrophobic surface chemistry together with large surface asperity, where air can be trapped between textured grooves, thus, dramatically decreasing the fraction of liquid‐solid contact. [ 7 ] However, when the pressure applied to water is greater than the critical pressure at the gas‐liquid interface, transition from the Cassie‐Baxter non‐wetting state to the Wenzel wetting state occurs, where water is impregnated into the surface textures and will not be able to overcome the energy barrier to return to the non‐wetting state without external simulate.…”
Section: Introductionmentioning
confidence: 99%