EXP 1-4 Measurement Data and Results: Difference between revisions
Line 16: | Line 16: | ||
Fig. 7 compares experimental results for the three crown dimensions (base diameter, rim diameter, crown height) with numerical results obtained for the two surface tension models and different grid resolution for the case with moderate impact energy. In contrast to the equilibrium model for surface tension, the relaxation model is able to reproduce the experimental data with reasonable accuracy irrespective of the number of interfacial cells. The Excel file for this case includes one worksheet for each | Fig. 7 compares experimental results for the three crown dimensions (base diameter, rim diameter, crown height) with numerical results obtained for the two surface tension models and different grid resolution for the case with moderate impact energy. In contrast to the equilibrium model for surface tension, the relaxation model is able to reproduce the experimental data with reasonable accuracy irrespective of the number of interfacial cells. The Excel file for this case includes one worksheet for each of the six subfigures of Fig. 7. Each of the six worksheets contains one column for time, one column for the respective measured (experimental) crown dimension and four columns for the respective numerical results obtained with the four different resolutions. | ||
Revision as of 07:16, 9 August 2023
Axisymmetric drop impact dynamics on a wall film of the same liquid
Measurement data/results
Excel files with experimental results for moderate and high impact velocity are available for download through the website https://tudatalib.ulb.tu-darmstadt.de/handle/tudatalib/3295 or via the following doi: https://doi.org/10.48328/tudatalib-722. In addition to the experimental results, the Excel files also include results of numerical simulations with a phase-field method. The content of the Excel files is described below.
In the numerical simulations, two different models for the surface tension force (equilibrium/relaxation) are employed in combination with different spatial resolutions. In the phase field method, the surface tension force is related to the profile of the phase-discriminating order parameter (C) and depends in particular on the gradient of C within the diffuse interface region. In the standard (equilibrium) formulation, C is assumed to follow the tanh profile of the equilibrium state whereas the relaxation model accounts for the deviation of the actual profile of C from the equilibrium profile. The spatial resolution is quantified by the number of mesh cells Nc used to resolve the diffuse interface as illustrated in Fig. 6.
Fig. 7 compares experimental results for the three crown dimensions (base diameter, rim diameter, crown height) with numerical results obtained for the two surface tension models and different grid resolution for the case with moderate impact energy. In contrast to the equilibrium model for surface tension, the relaxation model is able to reproduce the experimental data with reasonable accuracy irrespective of the number of interfacial cells. The Excel file for this case includes one worksheet for each of the six subfigures of Fig. 7. Each of the six worksheets contains one column for time, one column for the respective measured (experimental) crown dimension and four columns for the respective numerical results obtained with the four different resolutions.
A similar Excel file is provided for the case with high impact energy. A figure similar to Fig. 7 but for the high energy impact can found in the reference below, where besides a detailed discussion of the experimental and numerical results also conclusions drawn from the comparison are provided.
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
© copyright ERCOFTAC 2024