Phase diagram for droplet impact on superheated surfaces

We experimentally determine the phase diagram for impacting ethanol droplets on a smooth, sapphire surface in the parameter space of Weber number $\mathit{We}$ versus surface temperature $T$ . We observe two transitions, namely the one towards splashing (disintegration of the droplet) with increasin...

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Veröffentlicht in:Journal of fluid mechanics 2015-09, Vol.779, p.022104; 264501; 036302; 074503; 054501; 134502; 024507; 24001; 036101; 036310; 184505-022104; 264501; 036302; 074503; 054501; 134502; 024507; 24001; 036101; 036310; 184505, Article R3
Hauptverfasser: Staat, Hendrik J. J., Tran, Tuan, Geerdink, Bart, Riboux, Guillaume, Sun, Chao, Gordillo, José Manuel, Lohse, Detlef
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Sprache:eng
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Zusammenfassung:We experimentally determine the phase diagram for impacting ethanol droplets on a smooth, sapphire surface in the parameter space of Weber number $\mathit{We}$ versus surface temperature $T$ . We observe two transitions, namely the one towards splashing (disintegration of the droplet) with increasing $\mathit{We}$ , and the one towards the Leidenfrost state (no contact between the droplet and the plate due to a lasting vapour film) with increasing $T$ . Consequently, there are four regimes: contact and no splashing (deposition regime), contact and splashing (contact–splash regime), neither contact nor splashing (bounce regime), and finally no contact, but splashing (film–splash regime). While the transition temperature $T_{L}$ to the Leidenfrost state depends weakly, at most, on $\mathit{We}$ in the parameter regime of the present study, the transition Weber number $\mathit{We}_{C}$ towards splashing shows a strong dependence on $T$ and a discontinuity at $T_{L}$ . We quantitatively explain the splashing transition for $T
ISSN:0022-1120
1469-7645
DOI:10.1017/jfm.2015.465