Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces
False color environmental scanning electron microscope (ESEM) images of water freezing on smooth (θe ≈ 120°) and nanostructured (l ~ 50 nm, θe ≈ 170 - 180°) hydrophobic surfaces are presented. To obtain the freezing dynamics of water droplets, the vapor pressure in the ESEM chamber was set to 800 Pa...
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| Format: | Article |
| Language: | en_US |
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ASME International
2014
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| Online Access: | http://hdl.handle.net/1721.1/84997 https://orcid.org/0000-0001-7045-1200 |
| _version_ | 1826218028444942336 |
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| author | Miljkovic, Nenad Enright, Ryan Wang, Evelyn N. |
| author2 | Massachusetts Institute of Technology. Department of Mechanical Engineering |
| author_facet | Massachusetts Institute of Technology. Department of Mechanical Engineering Miljkovic, Nenad Enright, Ryan Wang, Evelyn N. |
| author_sort | Miljkovic, Nenad |
| collection | MIT |
| description | False color environmental scanning electron microscope (ESEM) images of water freezing on smooth (θe ≈ 120°) and nanostructured (l ~ 50 nm, θe ≈ 170 - 180°) hydrophobic surfaces are presented. To obtain the freezing dynamics of water droplets, the vapor pressure in the ESEM chamber was set to 800 Pa. The images were obtained with a beam potential of 20 kV and variable probe current. The surface temperature was initially set to 5 ± 1.5 °C using a cold stage, resulting in water droplet condensation. After a period of time, the surface temperature was decreased to -20 ± 1.5 °C, rapidly freezing the condensed droplets. The three images capture the freezing dynamics on hydrophobic and superhydrophobic surfaces. Figure 1a shows a snapshot of droplet coalescence between a large droplet (left) and a smaller droplet (right) on a nanostructured surface. Due to rapid freezing (Figure 1b), ice droplets maintained an ‘amorphous’ spherical structure (blue). Subsequent deposition of ice preferentially initiated on the droplet interface and formed crystallographic ice (red). Figure 2 shows a larger scale droplet (R ~ 100 μm) undergoing rapid freezing with notable protrusions. The heat flux (q” ~ 1 GW/m2) due to the latent heat of freezing could not be removed rapidly enough to match the velocity of the freezing front (vf ≈ 1500 m/s), resulting in evaporation and ejection of the liquid (protrusions) from the droplet interface. These distinct freezing droplet behaviors can significantly alter dynamics of phasechange phenomena on these surfaces. The visualizations provide insight into these complex droplet-surface interactions, which are important for the development of de-icing surfaces. |
| first_indexed | 2024-09-23T17:13:01Z |
| format | Article |
| id | mit-1721.1/84997 |
| institution | Massachusetts Institute of Technology |
| language | en_US |
| last_indexed | 2024-09-23T17:13:01Z |
| publishDate | 2014 |
| publisher | ASME International |
| record_format | dspace |
| spelling | mit-1721.1/849972022-10-03T11:10:28Z Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces Miljkovic, Nenad Enright, Ryan Wang, Evelyn N. Massachusetts Institute of Technology. Department of Mechanical Engineering Miljkovic, Nenad Miljkovic, Nenad Enright, Ryan Wang, Evelyn N. False color environmental scanning electron microscope (ESEM) images of water freezing on smooth (θe ≈ 120°) and nanostructured (l ~ 50 nm, θe ≈ 170 - 180°) hydrophobic surfaces are presented. To obtain the freezing dynamics of water droplets, the vapor pressure in the ESEM chamber was set to 800 Pa. The images were obtained with a beam potential of 20 kV and variable probe current. The surface temperature was initially set to 5 ± 1.5 °C using a cold stage, resulting in water droplet condensation. After a period of time, the surface temperature was decreased to -20 ± 1.5 °C, rapidly freezing the condensed droplets. The three images capture the freezing dynamics on hydrophobic and superhydrophobic surfaces. Figure 1a shows a snapshot of droplet coalescence between a large droplet (left) and a smaller droplet (right) on a nanostructured surface. Due to rapid freezing (Figure 1b), ice droplets maintained an ‘amorphous’ spherical structure (blue). Subsequent deposition of ice preferentially initiated on the droplet interface and formed crystallographic ice (red). Figure 2 shows a larger scale droplet (R ~ 100 μm) undergoing rapid freezing with notable protrusions. The heat flux (q” ~ 1 GW/m2) due to the latent heat of freezing could not be removed rapidly enough to match the velocity of the freezing front (vf ≈ 1500 m/s), resulting in evaporation and ejection of the liquid (protrusions) from the droplet interface. These distinct freezing droplet behaviors can significantly alter dynamics of phasechange phenomena on these surfaces. The visualizations provide insight into these complex droplet-surface interactions, which are important for the development of de-icing surfaces. 2014-02-19T14:21:32Z 2014-02-19T14:21:32Z 2012-06 Article http://purl.org/eprint/type/JournalArticle 00221481 http://hdl.handle.net/1721.1/84997 Miljkovic, Nenad, Ryan Enright, and Evelyn N Wang. “Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces.” Journal of Heat Transfer 134, no. 8 (2012): 080902. https://orcid.org/0000-0001-7045-1200 en_US http://dx.doi.org/10.1115/1.4006675 Journal of Heat Transfer Creative Commons Attribution-Noncommercial-Share Alike http://creativecommons.org/licenses/by-nc-sa/4.0/ application/pdf ASME International Nenad Miljkovic |
| spellingShingle | Miljkovic, Nenad Enright, Ryan Wang, Evelyn N. Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title | Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title_full | Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title_fullStr | Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title_full_unstemmed | Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title_short | Liquid Freezing Dynamics on Hydrophobic and Superhydrophobic Surfaces |
| title_sort | liquid freezing dynamics on hydrophobic and superhydrophobic surfaces |
| url | http://hdl.handle.net/1721.1/84997 https://orcid.org/0000-0001-7045-1200 |
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