Role of surface elasticity in the drainage of soap films

1993 ◽  
Vol 71 (14) ◽  
pp. 2342-2345 ◽  
Author(s):  
A. A. Sonin ◽  
A. Bonfillon ◽  
D. Langevin
1994 ◽  
Vol 162 (2) ◽  
pp. 323-330 ◽  
Author(s):  
A.A. Sonin ◽  
A. Bonfillon ◽  
D. Langevin
Keyword(s):  

2013 ◽  
Vol 739 ◽  
pp. 124-142 ◽  
Author(s):  
Jacopo Seiwert ◽  
Benjamin Dollet ◽  
Isabelle Cantat

AbstractIn this work, we study theoretically the thickness of a liquid film (typically made of a surfactant solution) pulled out of a bath at constant speed in the absence of gravity, when it features a viscous or an elastic interfacial rheology. We show that a purely viscous rheology does not lead to the extraction of a steady state film of constant thickness. In contrast, the thickness of the film is well defined in the elastic case, which allows us to compute it. This thickness depends on the capillary number of the experiment, and on the elasticity of the interface. It is always lower than or equal to that obtained for an incompressible interface predicted by Frankel (Mysels, Shinoda and Frankel, Soap Films: Studies of their Thinning and a Bibliography, 1959), which is recovered in the limit of an arbitrary large elasticity.


2015 ◽  
Vol 774 ◽  
Author(s):  
P. C. Petit ◽  
M. Le Merrer ◽  
A.-L. Biance

The classical problem of foam film rupture dynamics has been investigated when the film interfaces exhibit very high rigidity due to the presence of specific surfactants. Two new features are reported. First, a strong deviation from the well-known Taylor–Culick law is observed. Second, crack-like patterns can be visualized in the film; these patterns are shown to appear at a well-defined film shrinkage. The key role of surface-active material on these features is quantitatively investigated, pointing to the importance of surface elasticity to describe these fast dynamical processes and thus providing an alternative tool to characterize surface elasticity in conditions extremely far from equilibrium. The origin of the cracks and their consequences on film rupturing dynamics are also discussed.


2011 ◽  
Vol 22 (26) ◽  
pp. 265502 ◽  
Author(s):  
Mai Duc Dai ◽  
Chang-Wan Kim ◽  
Kilho Eom

Langmuir ◽  
2009 ◽  
Vol 25 (10) ◽  
pp. 5565-5573 ◽  
Author(s):  
Daniela Georgieva ◽  
Véronique Schmitt ◽  
Fernando Leal-Calderon ◽  
Dominique Langevin

2010 ◽  
Vol 652 ◽  
pp. 529-539 ◽  
Author(s):  
BENJAMIN DOLLET ◽  
ISABELLE CANTAT

The behaviour of soap films pushed through tubes at large velocities, up to several metres per second, is investigated in this paper. The film shape deviates from its equilibrium configuration perpendicular to the walls and gets curved downstream. A simple model relates the radius of curvature of the film to the friction in the lubrication films touching the wall, and the scaling of Bretherton (J. Fluid Mech., vol. 10, 1961, pp. 166–188) holds up to surprisingly high velocities, at which the capillary and Weber numbers are no longer small parameters. The tube geometry is varied and accounted for through the notion of hydraulic diameter. A limit of stability of the films, beyond which they burst or evolve unsteadily, is predicted, and it quantitatively captures the observations. The new questions raised by our results on the dissipation in soap films are discussed, especially the role of Plateau borders and inertial effects.


JAMA ◽  
1966 ◽  
Vol 195 (12) ◽  
pp. 1005-1009 ◽  
Author(s):  
D. J. Fernbach
Keyword(s):  

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