TY - JOUR
T1 - Freezing of micrometer-sized liquid droplets of pure water evaporatively cooled in a vacuum
AU - Ando, Kota
AU - Arakawa, Masashi
AU - Terasaki, Akira
N1 - Funding Information:
This work was supported by JSPS KAKENHI Grant Numbers JP23245006, JP26870431, JP15K13627, JP17H06456 and JP17K19017.
Publisher Copyright:
© 2018 the Owner Societies.
PY - 2018
Y1 - 2018
N2 - Freezing processes are reported for pure-water droplets generated in a vacuum in the size range of 49-71 μm in diameter. The process is characterized for each size by measurement of a freezing curve, where the fraction of frozen droplets is evaluated as a function of time. The 49 μm droplet was found to freeze at a time between 7.0 and 7.9 ms after being generated at room temperature, where the fraction of frozen droplets increased from 5% to 95%; the freezing time was thus distributed statistically within 1 ms. The freezing time was retarded by about 3 ms as the size increases from 49 to 71 μm, while the rise time of the freezing curve was almost unchanged. Numerical simulation of a cooling curve, i.e., the temperature of a droplet as a function of time, revealed that the droplets in the present size range are frozen at almost the same temperature between 233 and 236 K. The freezing curves measured in the experiment were well reproduced by numerical simulation based on the simulated cooling curves combined with the temperature dependence of the volume-based homogeneous ice nucleation rates of pure water reported previously. It was also found that a droplet is disintegrated into a few fragments upon freezing, which suggests formation of a frozen shell in the outer region of a droplet.
AB - Freezing processes are reported for pure-water droplets generated in a vacuum in the size range of 49-71 μm in diameter. The process is characterized for each size by measurement of a freezing curve, where the fraction of frozen droplets is evaluated as a function of time. The 49 μm droplet was found to freeze at a time between 7.0 and 7.9 ms after being generated at room temperature, where the fraction of frozen droplets increased from 5% to 95%; the freezing time was thus distributed statistically within 1 ms. The freezing time was retarded by about 3 ms as the size increases from 49 to 71 μm, while the rise time of the freezing curve was almost unchanged. Numerical simulation of a cooling curve, i.e., the temperature of a droplet as a function of time, revealed that the droplets in the present size range are frozen at almost the same temperature between 233 and 236 K. The freezing curves measured in the experiment were well reproduced by numerical simulation based on the simulated cooling curves combined with the temperature dependence of the volume-based homogeneous ice nucleation rates of pure water reported previously. It was also found that a droplet is disintegrated into a few fragments upon freezing, which suggests formation of a frozen shell in the outer region of a droplet.
UR - http://www.scopus.com/inward/record.url?scp=85056803995&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85056803995&partnerID=8YFLogxK
U2 - 10.1039/c8cp05955a
DO - 10.1039/c8cp05955a
M3 - Article
C2 - 30406234
AN - SCOPUS:85056803995
SN - 1463-9076
VL - 20
SP - 28435
EP - 28444
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
IS - 45
ER -