Droplet Boiling on Micro-Pillar Array Surface ─ Transition Boiling Regime
Droplet boiling on the heating surface is a representative phenomenon in two-phase spray cooling under low volumetric fluxes. In particular, droplet boiling in the transition boiling regime holds the advantages of avoiding heat transfer deterioration in a film boiling regime and achieving comparable...
| Veröffentlicht in: | Langmuir : the ACS journal of surfaces and colloids. - 1999. - 39(2023), 48 vom: 05. Dez., Seite 17392-17411 |
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| Format: | Online-Aufsatz |
| Sprache: | English |
| Veröffentlicht: |
2023
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| Zugriff auf das übergeordnete Werk: | Langmuir : the ACS journal of surfaces and colloids |
| Schlagworte: | Journal Article |
| Zusammenfassung: | Droplet boiling on the heating surface is a representative phenomenon in two-phase spray cooling under low volumetric fluxes. In particular, droplet boiling in the transition boiling regime holds the advantages of avoiding heat transfer deterioration in a film boiling regime and achieving comparable high heat transfer capacity in a nucleate boiling regime. While it is known to consist of intermittent liquid contact with the surface and surface dryout, quantifying the ensuing transient heat transfer performance and droplet behavior is very illusive. In this study, droplet boiling in the transition boiling regime on a micropillar array surface is investigated systematically, using the lattice Boltzmann model built up in the lab. The major contents discussed include the transient behaviors of the droplet, motion of the liquid bridge, and pinning/depinning of the three-phase contact line (TPCL), as well as the corresponding heat transfer performance. The evolution of a vapor film pierced by micropillars is analyzed from the views of morphological change and pressure distribution. The thickness of the vapor film is determined by the vapor generation rate dominated by the contact area and effective thermal conductivity, and the vapor escape rate by the permeability. The low permeability under a large pillar side length is responsible for the pressure buildup below the droplet, thus facilitating droplet rebound. The competition between capillary pressure and vapor film pressure dominates the trigger mode of the droplet rebound, i.e., fracture of the liquid bridge or filament and depinning of TPCL. The micropillar array surface is optimized to pursue the best cooling performance by assessing the impact from micropillar geometric dimensions on droplet contact time and area |
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| Beschreibung: | Date Revised 05.12.2023 published: Print-Electronic Citation Status PubMed-not-MEDLINE |
| ISSN: | 1520-5827 |
| DOI: | 10.1021/acs.langmuir.3c02550 |