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Soap films are thin layers of liquid (usually water-based) surrounded by air. For example, if two soap bubbles come into contact, they merge and a thin film is created in between. Thus, foams are composed of a network of films connected by Plateau borders. Films are used as model systems for minimal surfaces, which are widely used in mathematics. Flowing soap film has been used to study two-dimensional turbulence, and serves as a water tunnel to study flow-structure interactions. One notable example was the study of a flapping flag in the wind, which could be demonstrated as a "2D wind" of flowing soap film passing by a silk thread that acts as a flexible flag. Due to the thinness of the films, flow visualization using interferometry could reveal great flow details.

Stability

Daily experience shows that soap bubble formation is not feasible with water or with any pure liquid. Actually, the presence of soap, which is composed at a molecular scale of surfactants, is necessary to stabilize the film. Most of the time, surfactants are amphiphilic, which means they are molecules with both a hydrophobic and a hydrophilic part. Thus, they are arranged preferentially at the air/water interface (see figure 1).

Surfactants stabilize films because they create a repulsion between both surfaces of the film, preventing it from thinning and consequentially bursting. This can be shown quantitatively through calculations relating to disjoining pressure. The main repulsion mechanisms are steric (the surfactants can not interlace) and electrostatic (if surfactants are charged).

Moreover, surfactants make the film more stable toward thickness fluctuations due to the Marangoni effect. This gives some elasticity to the interface: if surface concentrations are not homogeneously dispersed at the surface, Marangoni forces will tend to re-homogenize the surface concentration (see figure 2).

Even in the presence of stabilizing surfactants, a soap film does not last forever. Water evaporates with time depending on the humidity of the atmosphere. Moreover, as soon as a film is not perfectly horizontal, the liquid flows toward the bottom due to gravity and the liquid accumulates at the bottom. At the top, the film thins and bursts.

Importance of surface tension: minimal surfaces

From a mathematical point of view, soap films are considered minimal surfaces. See for instance the approximate numerical method for minimal surfaces form finding at Stretched grid method. Surface tension, which measures the energy needed to create a surface indeed acts as a physical surface minimizer: since surface energy is proportional to the soap film surface, the film deforms to minimize its surface and, thus its energy.

Depending on the support provided, the soap film naturally takes the minimal surface. On a flat support, the soap film is usually flat. But, on more complicate supports, it takes the minimal achievable surface.

Colours

The iridescent colours of a soap film are caused by interfering of (internally and externally) reflected light waves, a process called thin film interference and are determined by the thickness of the film. This phenomenon is not the same as the origin of rainbow colours (caused by the refraction of internally reflected light), but rather is the same as the phenomenon causing the colours in an oil slick on a wet road.

Drainage

If surfactants are well chosen and the atmospheric humidity and air movements are suitably controlled, a horizontal soap film can last from minutes to hours. In contrast, a vertical soap film is affected by gravity and so the liquid tends to drain, causing the soap film to thin at the top. Colour depends on film thickness, which accounts for the coloured interference fringes that can be seen at the top of figure 4.

Bursting

If a soap film is unstable, it ends by bursting. A hole is created somewhere in the film and opens very rapidly. Surface tension indeed leads to surface minimization and, thus, to film disappearance. The hole aperture is not instantaneous and is slowed by the liquid inertia. The balance between the forces of inertia and surface tension leads to the opening velocity: ${\displaystyle V={\sqrt {\frac {2\gamma }{\rho h}}}}$ where ${\displaystyle \gamma }$ is the liquid surface tension, ${\displaystyle \rho }$ is the liquid density and ${\displaystyle h}$ is the film thickness.

References

1. ^ Ball, 2009. pp. 61–67
2. Culick, F. E. C. (1960). "Comments on a Ruptured Soap Film". Journal of Applied Physics. 31 (6). AIP Publishing: 1128–1129. doi:10.1063/1.1735765. ISSN 0021-8979.

General sources

• Ball, Philip (2009). Shapes. Nature's Patterns: a tapestry in three parts. Oxford University Press. pp. 61–67, 81–97, 291–292. ISBN 978-0-19-960486-9.

• Minimal surfaces
• Bubbles (physics)