Abstract

In this paper, the impact of a three-dimensional droplet falling on a hot surface above the Leidenfrost temperature is investigated by a volume-of-fluid based Navier–Stokes solver for liquid–vapour flows with phase change. The applicability of the direct numerical simulation (DNS) to capture the vapour film under an evaporating droplet is validated by favourable comparisons with static measurement results in experiments. Using this DNS method, the oscillation of the vapour pocket of a saturated Leidenfrost drop is studied in the rebounding stage, which provides important information about the transient heat transfer. By probing the evaporation and energy characteristics as well as the heat flow in the vapour layer, we reveal that the strong surface energy dominates the droplet morphology, and the bottom interface oscillation is mainly ascribed to the evaporation and lubrication effects. The effects of the governing dimensionless numbers indicate that increasing We (Weber number, inertia to surface tension) or Ja (Jakob number, sensible heat to latent heat) will intensify the bottom interface oscillation. In addition, the maximum spread factor of the impacting Leidenfrost drops has the scaling of ∼We1/4, according well with recent experiments. Our results further show that for rebounding drops with a small We, the non-dimensional maximal vapour pocket width and oscillation time interval are linear functions of We1/2 and We3/4, respectively. These relations facilitate the flow physics for dynamical Leidenfrost events and therefore, will guide the applications in the future.

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