Laser-driven droplet deformation at low Weber numbers

We investigate droplet deformation following laser-pulse impact at low Weber numbers ( ${\textit{We}}\sim 0.1{-}100$ ). Droplet dynamics can be characterised by two key parameters: the impact Weber number and the width, W , of the distribution of the impact force over the droplet surface. By varying laser-pulse energy, our experiments traverse a phase space comprising (i) droplet oscillation, (ii) breakup or (iii) sheet formation. Numerical simulations complement the experiments by determining the pressure width and by allowing We and W to be varied independently, despite their correlation in the experiments. A single phase diagram, integrating observations from both experiments and simulations, demonstrates that all phenomena can be explained by a single parameter: the deformation Weber number ${\textit{We}}_{{d}}=f({\textit{We}},{W})$ that is based on the initial radial expansion speed of the droplet, following impact. The resulting phase diagram separates (i) droplet oscillation for ${\textit{We}}_{{d}}\lt 5$ , from (ii) breakup for $5\lt {\textit{We}}_{{d}}\lt 60$ and (iii) sheet formation for ${\textit{We}}_{{d}}\gt 60$ .

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Publication Details

Journal
Journal of Fluid Mechanics
Published
2026-04-28
DOI
https://doi.org/10.1017/jfm.2026.11470
Primary Topic
Fluid Dynamics and Heat Transfer
Type
article
Field-Weighted Citation Impact
0.00

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article

Laser-driven droplet deformation at low Weber numbers

Maziyar Jalaal, H. K. Schubert, Mikheil Kharbedia, Oscar Versolato et al.
Journal of Fluid Mechanics
Fluid Dynamics and Heat Transfer
article

Laser-driven droplet deformation at low Weber numbers

Maziyar Jalaal, H. K. Schubert, Mikheil Kharbedia, Oscar Versolato, Hugo França, Dion Engels
article en

Abstract

We investigate droplet deformation following laser-pulse impact at low Weber numbers ( ${\textit{We}}\sim 0.1{-}100$ ). Droplet dynamics can be characterised by two key parameters: the impact Weber number and the width, W , of the distribution of the impact force over the droplet surface. By varying laser-pulse energy, our experiments traverse a phase space comprising (i) droplet oscillation, (ii) breakup or (iii) sheet formation. Numerical simulations complement the experiments by determining the pressure width and by allowing We and W to be varied independently, despite their correlation in the experiments. A single phase diagram, integrating observations from both experiments and simulations, demonstrates that all phenomena can be explained by a single parameter: the deformation Weber number ${\textit{We}}_{{d}}=f({\textit{We}},{W})$ that is based on the initial radial expansion speed of the droplet, following impact. The resulting phase diagram separates (i) droplet oscillation for ${\textit{We}}_{{d}}\lt 5$ , from (ii) breakup for $5\lt {\textit{We}}_{{d}}\lt 60$ and (iii) sheet formation for ${\textit{We}}_{{d}}\gt 60$ .

Journal of Fluid MechanicsVol. 1034
Advanced Research Center for Nanolithography (Netherlands) (NL), Vrije Universiteit Amsterdam (NL), University of Amsterdam (NL)
European Commission, Rijksuniversiteit Groningen, Universiteit van Amsterdam, Vrije Universiteit Amsterdam, Nederlandse Organisatie voor Wetenschappelijk Onderzoek, Ministerie van Economische Zaken en Klimaat, Topconsortium voor Kennis en Innovatie, H2020 European Research Council
Openalex Percentile: Top 5%
Fluid Dynamics and Heat Transfer
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