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Abstracts - KTH Mechanics

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30<br />

Dynamic wetting transition: avoided critical behavior<br />

G. Delon ∗ , J.H. Snoeijer ∗ ,B. Andreotti ∗ and M. Fermigier ∗<br />

A solid surface can be coated by a thin film when the solid is withdrawn at<br />

constant speed out of a bath of liquid. This dip coating process was analyzed initially<br />

by Landau-Levich.<br />

In a partial wetting situation, there is a threshold velocity below which the meniscusissteadyandthesolidremainsdry.<br />

We investigate the dynamic wetting transition<br />

between the two states : at low velocity, a stable meniscus, at high velocity, an entrained<br />

film.<br />

It has been shown that a receding contact line becomes unstable when the capillary<br />

number exceeds a critical value Cac 1 . In our experiments, liquid entrainment occurs<br />

at a capillary number Ca ∗ which is lower than Cac. The critical behavior expected at<br />

Cac is thus avoided. The threshold velocity coincides precisely with the contact line<br />

velocity above the transition. We explain the occurence of an early transition by the<br />

nucleation of a a capillary ridge (see fig.) which moves ahead of the thin film. The<br />

characteristics of this ridge determine the threshold velocity for liquid entrainment.<br />

We discuss also the influence of the curvature of the solid surface on the wetting<br />

transition.<br />

∗ PMMH,ESPCI, 10 rue Vauquelin, 75005 Paris, France.<br />

1 J. Eggers Phys. Fluids 17, 082106 (2005).<br />

8<br />

z (cm)<br />

7<br />

6<br />

5<br />

U p<br />

100 µm<br />

Figure 1: (Left) Liquid film (brighter part) entrained by a vertical plate pulled out<br />

of bath of silicone oil. (Right) Time evolution of the ridge profile (vertical cross<br />

sections in the middle of the liquid film. The three oblique lines in this space-time<br />

diagram represent the velocity of the solid plate, the velocity of the contact line and<br />

the velocity of the front between ridge and thin film.<br />

0<br />

100<br />

200<br />

U cl<br />

300<br />

U j<br />

400<br />

t (s)

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