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scienceMonday, July 13, 2026 at 04:01 PM
Simulations establish self-similar Worthington jet collapse with r_j scaling as tau^0.63, driving local Weber number to infinity

Simulations establish self-similar Worthington jet collapse with r_j scaling as tau^0.63, driving local Weber number to infinity

High-fidelity simulations of bursting micron bubbles reveal that Worthington jets are governed by a beta-dependent self-similar solution in which jet radius scales as tau^0.63 and local Weber number diverges. The work predicts nanometric initial jet radii and universal interface shapes over two decades in time. This inertial dominance revises estimates of sea-spray aerosol production from bubble bursting.

The arXiv preprint by Sanjay et al. solves the axisymmetric Euler equations with free-surface boundary conditions for a conical cavity formed after bubble rupture. Local collapse is controlled solely by the opening semi-angle beta, yielding a universal interface shape when lengths are nondimensionalized by the predicted r_j(tau). This scaling holds independently of viscosity and far-field conditions once inertial focusing begins.

Earlier experiments on drop-impact Worthington jets reported similar thin spikes but lacked the temporal resolution to test the predicted exponent or the divergence of We_j. The new work closes that gap by showing that capillary regularization is overwhelmed at radii below 10 nm in water, directly implying the ejection of sea-spray aerosols whose initial size is set by the inertial singularity rather than by equilibrium surface tension.

The result connects to broader patterns in singular free-surface flows, including the conical shapes seen in bubble entrainment and electrospray. It suggests that aerosol generation models must incorporate this inertial-focusing regime rather than assuming a fixed minimum neck radius.

⚡ Prediction

Vatsal Sanjay: High-speed interferometric measurements will recover the 0.63 exponent for jet radius down to 50 nm within 18 months.

Sources (2)

  • [1]
    Primary Source(https://arxiv.org/abs/2607.08972)
  • [2]
    Supporting Source(https://doi.org/10.1017/jfm.2019.1023)