Condensation on Hydrophilic, Hydrophobic, Nanostructured Superhydrophobic and Oil-Infused Surfaces
Name
Condensation on Hydrophilic, Hydrophobic, Nanostructured Superhydrophobic and Oil-Infused Surfaces.pdf
Description
Main article, figures, and supplementary information
Size
1.11 MB
Format
Adobe PDF
Checksum (MD5)
14e88ccd9e6d876bee32269980186a0b
Author(s)
Nenad, Miljkovic
Rong, Xiao
Ryan, Enright
Ian, McKay
Preston, Daniel John
Wang, Evelyn N.
Miljkovic, Nenad
Xiao, Rong
Enright, Ryan
McKay, Ian
Date Issued
July 2013
Journal
Journal of Heat Transfer
Publisher
ASME International
Citation
Nenad, Miljkovic et al. “Condensation on Hydrophilic, Hydrophobic, Nanostructured Superhydrophobic and Oil-Infused Surfaces.” Journal of Heat Transfer 135.8 (2013): 080906.
Version
Author's final manuscript
Abstract
Color images of steady state water vapor condensing on smooth and nanostructured hydrophobic surfaces are presented. Figure 1a shows a snapshot of classical filmwise condensation on hydrophilic copper. A thin liquid film forms on the high surface energy substrate and acts as a conduction barrier for heat transfer. Figure 1b shows dropwise condensation on a copper tube made hydrophobic via deposition of a tri-chloro silane (TFTS). Discrete droplets form on the surface and, upon reaching a size comparable to the capillary length (≈2.7 mm), depart from the surface by gravitational sweeping. Figure 1c shows jumping-droplet condensation on a nanostructured superhydrophobic copper oxide (CuO) surface. When droplets coalesce on this surface, the resulting droplet can jump due to the release of excess surface energy (Figure 2b), and as a result, rapid droplet jumping is observed at micrometric length scales (R < 20 μm). Figure 1d shows a novel mode of condensation called ‘immersion’ condensation, where nucleation density is drastically increased while maintaining easy condensate removal (R < 500 μm) and low contact angles (<120˚). This approach utilizes an oil-infused nanostructured CuO surface with a heterogeneous coating which allows droplets to nucleate immersed within the oil (Figure 2c). The increase in nucleation density is achieved due to the combined effect of surface energy heterogeneity and a reduced oil-water interfacial energy. Figure 2a shows a schematic of the experimental setup. The visualizations provide insight into the complex droplet-surface interactions, which are important for the development of enhanced phase change surfaces. If designed properly, these surfaces not only allow for easy droplet removal at micrometric length scales during condensation but also promise to enhance heat transfer performance.
MIT Department
Massachusetts Institute of Technology. Department of Mechanical Engineering
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Creative Commons Attribution-Noncommercial-Share Alike
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DOI of Published Version
https://doi.org/10.1115/1.4024188
