Evaporation of Condensate Droplets on Structured Surfaces with Gradient RoughnessSource: Journal of Heat Transfer:;2015:;volume( 137 ):;issue: 008::page 80903DOI: 10.1115/1.4030449Publisher: The American Society of Mechanical Engineers (ASME)
Abstract: The study of evaporation dynamics of droplets is of scientific interest and has numerous practical applications. Here, we studied the evaporation of small condensate droplets on structured surfaces with onetier microscale roughness and twotier micro/nanoscale roughness (the top and valley of micropillars are covered by nanograss), respectively. On both surfaces, the micropillar arrays are arranged in a radical lattice with the decreasing pillartopillar spacing towards the center of the surface (The first figures in Figs. 1 and 2). The condensate droplets on structured surfaces were formed by conducting condensation inside environmental scanning electron microscope (ESEM, Philips XL30, ~4.9 Torr, stage temperature ~ 3آ°C). The condensate droplet on the onetier surface stays in a Cassiestate (0 s in Fig. 1). However, owing to the preferential droplet nucleation on the smooth sidewall of micropillars, the condensate droplet on the twotier surface maintains in the composite state (0 s in Fig. 2). To visualize the evaporation dynamics of condensate droplet, we gradually decreased the vapor pressure in the chamber from ~4.9 Torr to ~4.2 Torr. On the onetier surface (Fig. 1), the droplet first evaporates in a constant contact radius mode (CCR, 0124 s), followed by a constant contact angle mode (CCA, 136166 s), and a mixed mode of both CCR and CCA (188224 s). By contrast, on the twotier surface (Fig. 2), the condensate droplet first evaporates in the CCR mode, with the solidliquid contact line remain pinned until the formation of a flat liquidair interface at the top of micropillars at ~86 s. After that, the liquidair interface at the top of surface remains flat and the liquid evaporation is dominant in the lateral direction (96170 s), with the liquid cylinder symmetrically shrinking towards the center of the surface. The presence of a stable and flat liquid/air interface at the top of surface is due to the stabilization effect rendered by the nanograss on the micropillars.
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| contributor author | Chen, Xuemei | |
| contributor author | Yao, Shuhuai | |
| contributor author | Wang, Zuankai | |
| date accessioned | 2017-05-09T01:19:48Z | |
| date available | 2017-05-09T01:19:48Z | |
| date issued | 2015 | |
| identifier issn | 0022-1481 | |
| identifier other | ht_137_08_080903.pdf | |
| identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/158515 | |
| description abstract | The study of evaporation dynamics of droplets is of scientific interest and has numerous practical applications. Here, we studied the evaporation of small condensate droplets on structured surfaces with onetier microscale roughness and twotier micro/nanoscale roughness (the top and valley of micropillars are covered by nanograss), respectively. On both surfaces, the micropillar arrays are arranged in a radical lattice with the decreasing pillartopillar spacing towards the center of the surface (The first figures in Figs. 1 and 2). The condensate droplets on structured surfaces were formed by conducting condensation inside environmental scanning electron microscope (ESEM, Philips XL30, ~4.9 Torr, stage temperature ~ 3آ°C). The condensate droplet on the onetier surface stays in a Cassiestate (0 s in Fig. 1). However, owing to the preferential droplet nucleation on the smooth sidewall of micropillars, the condensate droplet on the twotier surface maintains in the composite state (0 s in Fig. 2). To visualize the evaporation dynamics of condensate droplet, we gradually decreased the vapor pressure in the chamber from ~4.9 Torr to ~4.2 Torr. On the onetier surface (Fig. 1), the droplet first evaporates in a constant contact radius mode (CCR, 0124 s), followed by a constant contact angle mode (CCA, 136166 s), and a mixed mode of both CCR and CCA (188224 s). By contrast, on the twotier surface (Fig. 2), the condensate droplet first evaporates in the CCR mode, with the solidliquid contact line remain pinned until the formation of a flat liquidair interface at the top of micropillars at ~86 s. After that, the liquidair interface at the top of surface remains flat and the liquid evaporation is dominant in the lateral direction (96170 s), with the liquid cylinder symmetrically shrinking towards the center of the surface. The presence of a stable and flat liquid/air interface at the top of surface is due to the stabilization effect rendered by the nanograss on the micropillars. | |
| publisher | The American Society of Mechanical Engineers (ASME) | |
| title | Evaporation of Condensate Droplets on Structured Surfaces with Gradient Roughness | |
| type | Journal Paper | |
| journal volume | 137 | |
| journal issue | 8 | |
| journal title | Journal of Heat Transfer | |
| identifier doi | 10.1115/1.4030449 | |
| journal fristpage | 80903 | |
| journal lastpage | 80903 | |
| identifier eissn | 1528-8943 | |
| tree | Journal of Heat Transfer:;2015:;volume( 137 ):;issue: 008 | |
| contenttype | Fulltext |