Related Experiment Video
Updated: Mar 31, 2026

Measuring the Interaction Force Between a Droplet and a Super-hydrophobic Substrate by the Optical Lever Method
Published on: June 14, 2019
Lattice Boltzmann modeling of self-propelled Leidenfrost droplets on ratchet surfaces
Qing Li1, Q J Kang2, M M Francois3
1School of Energy Science and Engineering, Central South University, Changsha 410083, China and Computational Earth Science Group, Los Alamos National Laboratory, Los Alamos, NM 87545, USA. qkang@lanl.gov.
Abstract:
In this paper, the self-propelled motion of Leidenfrost droplets on ratchet surfaces is numerically investigated using a thermal multiphase lattice Boltzmann model with liquid-vapor phase change. The capability of the model for simulating evaporation is validated via the D(2) law. Using the model, we first study the performances of Leidenfrost droplets on horizontal ratchet surfaces. It is numerically shown that the motion of self-propelled Leidenfrost droplets on ratchet surfaces is owing to the asymmetry of the ratchets and the vapor flows beneath the droplets. It is found that the Leidenfrost droplets move in the direction toward the slowly inclined side from the ratchet peaks, which agrees with the direction of droplet motion in experiments [Linke et al., Phys. Rev. Lett., 2006, 96, 154502]. Moreover, the influences of the ratchet aspect ratio are investigated. For the considered ratchet surfaces, a critical value of the ratchet aspect ratio is approximately found, which corresponds to the maximum droplet moving velocity. Furthermore, the processes that the Leidenfrost droplets climb uphill on inclined ratchet surfaces are also studied. Numerical results show that the maximum inclination angle at which a Leidenfrost droplet can still climb uphill successfully is affected by the initial radius of the droplet.
Related Concept Videos
Surface Tension of Fluid
Surface tension varies...
Steady, Laminar Flow Between Parallel Plates
Maxwell-Boltzmann Distribution: Problem Solving
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
Distribution of Molecular Speeds
Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model
Hydrostatic Pressure Force on a Curved Surface

