TY - JOUR
T1 - Leidenfrost Droplets on Microstructured Surfaces
AU - Duursma, Gail
AU - Kennedy, Ross
AU - Sefiane, Khellil
AU - Yu, Yong
N1 - Publisher Copyright:
© 2016 Taylor and Francis Group, LLC.
PY - 2016/9/21
Y1 - 2016/9/21
N2 - The lifetime of a droplet deposited on a hot plate decreases when the temperature of the plate increases, but above the critical Leidenfrost temperature, the lifetime suddenly increases. This is due to the formation of a thin layer of vapor between the droplet and the substrate, which plays a double role: First, it thermally insulates the droplet from the plate, and second, it allows the droplet to "levitate." The Leidenfrost point is affected by the roughness or microstructure of the surface. In this work, a silicon surface with different microstructured regions of square pillars was prepared such that there is a sharp transition (boundary) between areas of different pillar spacing. The Leidenfrost point was identified in experiments using water droplets ranging in size from 8 to 24 l and the behavior of the droplets was recorded using high-speed digital photography. The Leidenfrost point was found to vary by up to 120°C for pillar spacings from 10 to 100 m. If the droplet is placed on the boundary between structured sections, the droplet becomes asymmetric and may move or spin. An axisymmetric computational fluid dynamics (CFD) model is also presented that shows qualitative agreement with experimental observations.
AB - The lifetime of a droplet deposited on a hot plate decreases when the temperature of the plate increases, but above the critical Leidenfrost temperature, the lifetime suddenly increases. This is due to the formation of a thin layer of vapor between the droplet and the substrate, which plays a double role: First, it thermally insulates the droplet from the plate, and second, it allows the droplet to "levitate." The Leidenfrost point is affected by the roughness or microstructure of the surface. In this work, a silicon surface with different microstructured regions of square pillars was prepared such that there is a sharp transition (boundary) between areas of different pillar spacing. The Leidenfrost point was identified in experiments using water droplets ranging in size from 8 to 24 l and the behavior of the droplets was recorded using high-speed digital photography. The Leidenfrost point was found to vary by up to 120°C for pillar spacings from 10 to 100 m. If the droplet is placed on the boundary between structured sections, the droplet becomes asymmetric and may move or spin. An axisymmetric computational fluid dynamics (CFD) model is also presented that shows qualitative agreement with experimental observations.
UR - http://www.scopus.com/inward/record.url?scp=84961707347&partnerID=8YFLogxK
U2 - 10.1080/01457632.2015.1112610
DO - 10.1080/01457632.2015.1112610
M3 - Article
AN - SCOPUS:84961707347
SN - 0145-7632
VL - 37
SP - 1190
EP - 1200
JO - Heat Transfer Engineering
JF - Heat Transfer Engineering
IS - 13-14
ER -