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Initial solidification dynamics of spreading droplets

Robin B. J. Koldeweij1,2,*, Pallav Kant1, Kirsten Harth1,3, Rielle de Ruiter4, Hanneke Gelderblom5, Jacco H. Snoeijer1, Detlef Lohse1,6, and Michiel A. J. van Limbeek1,6

  • 1Physics of Fluids Group, Department of Science and Technology, Max Planck Center Twente for Complex Fluid Dynamics, J. M. Burgers Center for Fluid Dynamics, University of Twente, 7500 AE Enschede, The Netherlands
  • 2Nano-Instrumentation, TNO, 5612 AP Eindhoven, The Netherlands
  • 3Institute for Physics, Otto von Guericke University Magdeburg, 39106 Magdeburg, Germany
  • 4ASML, 5503 LA Veldhoven, The Netherlands
  • 5Department of Applied Physics, Eindhoven University of Technology, 5600 MB Eindhoven, Netherlands
  • 6Dynamics of Complex Fluids, Max Planck Institute for Dynamics and Self-Organization, 37077 Göttingen, Germany

  • *Corresponding author. robin.koldeweij@tno.nl

Phys. Rev. Fluids 6, L121601 – Published 3 December, 2021

DOI: https://doi.org/10.1103/PhysRevFluids.6.L121601

Abstract

When a droplet is brought in contact with an undercooled surface, it wets the substrate and solidifies at the same time. The interplay between the phase transition effects and the contact-line motion, leading to its arrest, remains poorly understood. Here we reveal the early solidification patterns and dynamics of spreading hexadecane droplets. Total internal reflection imaging is employed to temporally and spatially resolve the early solidification behavior. With this, we determine the conditions leading to the contact-line arrest. We quantify the overall nucleation behavior, i.e., the nucleation rate and the crystal growth speed and show its sensitivity to the applied undercooling of the substrate. We also show that for strong enough undercooling it is the rapid growth of the crystals which determines the eventual arrest of the spreading contact line. By combining the Johnson-Mehl-Avrami-Kolmogorov nucleation theory and scaling relations for the spreading, we calculate the temporal evolution of the solid area fraction, which is in good agreement with our observations.

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