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Capillary collapse of a bursting bubble is a canonical inertio-capillary singularity: the retracting rim launches a wave packet that focuses at the cavity base, driving a high-speed Worthington jet and, classically, droplets. Non-Newtonian physics rewrites this script. For example, yield stress and elasticity tame these waves and the jet and often suppress them [1]. Using high-fidelity simulations carried out with MultiRheoFlow (https://comphy-lab.org/MultiRheoFlow/)

Fig. Worthington jet vs. elastoviscoplastic medium, adapted from [1].
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Posted by:: Vatsal Date published:: 2025-06-09
Date modified:: Jun 9, 2025 at 20:28 CET
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References
[1] A. G. Balasubramanian, V. Sanjay, M. Jalaal, R. Vinuesa, and O. Tammisola, “Bursting bubble in an elasto-viscoplastic medium,” J. Fluid Mech., vol. 1001, p. A9, Dec. 2024, doi: 10.1017/jfm.2024.1073
[2] V. Sanjay, D. Lohse, and M. Jalaal, “Bursting bubble in a viscoplastic medium,” J. Fluid Mech., vol. 922, p. A2, 2021, doi: 10.1017/jfm.2021.489
[3] A. K. Dixit, A. Oratis, K. Zinelis, D. Lohse, and V. Sanjay, “Viscoelastic Worthington jets and droplets produced by bursting bubbles,” J. Fluid Mech., vol. 1010, p. A2, May 2025, doi: 10.1017/jfm.2025.237.
