TY - JOUR
T1 - Motion of Leidenfrost self-propelled droplets on ratchet in low- and high-temperature regimes
AU - Jo, Daeseong
N1 - Publisher Copyright:
© 2023, The Korean Society of Mechanical Engineers and Springer-Verlag GmbH Germany, part of Springer Nature.
PY - 2023/10
Y1 - 2023/10
N2 - Leidenfrost droplet experiments were conducted to investigate the movement of droplets on a ratchet in low- and high-temperature regimes (L and H regimes). Slightly above the threshold temperature, the terminal velocity increased with increasing temperature until it reached the highest value. After achieving the highest value, the terminal velocity gradually decreased with temperature until there was a significant decrease in the terminal velocity. Leidenfrost regimes were identified based on not only the droplet velocity but also the droplet shape and motion. In the H regime, there was a complete thin vapor film underneath the droplets, which caused them to levitate from the ratchet. However, in the L regime, there was no a complete vapor film underneath the droplets, causing direct contact between the droplets and ratchet, resulting in drastic nucleate boiling. This resulted in a faster vapor flow and generated a stronger rotational motion than that in the H regime. A stronger rotational motion results in a faster velocity in the translational direction.
AB - Leidenfrost droplet experiments were conducted to investigate the movement of droplets on a ratchet in low- and high-temperature regimes (L and H regimes). Slightly above the threshold temperature, the terminal velocity increased with increasing temperature until it reached the highest value. After achieving the highest value, the terminal velocity gradually decreased with temperature until there was a significant decrease in the terminal velocity. Leidenfrost regimes were identified based on not only the droplet velocity but also the droplet shape and motion. In the H regime, there was a complete thin vapor film underneath the droplets, which caused them to levitate from the ratchet. However, in the L regime, there was no a complete vapor film underneath the droplets, causing direct contact between the droplets and ratchet, resulting in drastic nucleate boiling. This resulted in a faster vapor flow and generated a stronger rotational motion than that in the H regime. A stronger rotational motion results in a faster velocity in the translational direction.
KW - Leidenfrost effect
KW - Rotational motion
KW - Self-propelled droplet
KW - Temperature regime
KW - Terminal velocity
UR - http://www.scopus.com/inward/record.url?scp=85173738268&partnerID=8YFLogxK
U2 - 10.1007/s12206-023-0941-4
DO - 10.1007/s12206-023-0941-4
M3 - Article
AN - SCOPUS:85173738268
SN - 1738-494X
VL - 37
SP - 5425
EP - 5430
JO - Journal of Mechanical Science and Technology
JF - Journal of Mechanical Science and Technology
IS - 10
ER -