EXP 1-4 Introduction: Difference between revisions
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The formation and expansion of the crown and the associated flow field in both phases are illustrated in Fig. 2 showing results of accompanying numerical simulations. Experimental videos of the drop-film interaction are provided for download in Section [[Lib:EXP 1-4 Description]]. From these videos, experimental data for the time evolution of the three characteristic dimensions of the crown are extracted, namely the height of the crown and its top and base radius (see Section [[Lib:EXP 1-4 Measurement Quantities and Techniques]].). | The formation and expansion of the crown and the associated flow field in both phases are illustrated in Fig. 2 showing results of accompanying numerical simulations. Experimental videos of the drop-film interaction are provided for download in Section [[Lib:EXP 1-4 Description]]. From these videos, experimental data for the time evolution of the three characteristic dimensions of the crown are extracted, namely the height of the crown and its top and base radius (see Section [[Lib:EXP 1-4 Measurement Quantities and Techniques]].). | ||
Further details can be found in the following publication: | |||
M. Bagheri, B. Stumpf, I.V. Roisman, C. Tropea, J. Hussong, M. Wörner, H. Marschall, Interfacial relaxation – Crucial for phase-field methods to capture low to high energy drop-film impacts, Int. J. Heat Fluid Flow 94 (2022) 108943, https://doi.org/10.1016/j.ijheatfluidflow.2022.108943 | |||
Revision as of 08:05, 10 August 2023
Axisymmetric drop impact dynamics on a wall film of the same liquid
Introduction
Droplet impact onto wetted surfaces is of pertinence to many technical applications such as internal combustion engines, icing on plane wings and spray coating technologies to name a few. Immediately after the impact, the droplet expands radially along the surface. If the impact kinetic energy is sufficiently high, an upward growing crown is generated with detachment of secondary droplets. For the cases considered here, splashing is absent and the drop-film interaction is axisymmetric. The two-phase flow is laminar and its dynamics is governed by an interplay between inertial, viscous and capillary forces.
The formation and expansion of the crown and the associated flow field in both phases are illustrated in Fig. 2 showing results of accompanying numerical simulations. Experimental videos of the drop-film interaction are provided for download in Section Lib:EXP 1-4 Description. From these videos, experimental data for the time evolution of the three characteristic dimensions of the crown are extracted, namely the height of the crown and its top and base radius (see Section Lib:EXP 1-4 Measurement Quantities and Techniques.).
Further details can be found in the following publication:
M. Bagheri, B. Stumpf, I.V. Roisman, C. Tropea, J. Hussong, M. Wörner, H. Marschall, Interfacial relaxation – Crucial for phase-field methods to capture low to high energy drop-film impacts, Int. J. Heat Fluid Flow 94 (2022) 108943, https://doi.org/10.1016/j.ijheatfluidflow.2022.108943
Contributed by: Milad Bagheri, Bastian Stumpf, Ilia V. Roisman, Cameron Tropea, Jeanette Hussong, Martin Wörner, Holger Marschall — Technical University of Darmstadt and Karlsruhe Institute of Technology
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