The spreading of a liquid on a surface occures in many physical problems, ranging from the protection of microchips to the build-up of ice on an airplane wing. On the theoretical side the dynamics of the thin films raise interesting questions involving the physics of different length scales. There are three significant length scales corresponding to (1) gravity, (2) surface tension, and (3) the relevant physics at the "contact line" or triple juncture of the three interfaces (liquid/air, liquid/solid, and solid/air). In Project Afton we will develop methods for visualizing flows driven by gravity, surface tension, and the interactions between the two.
The first is the rotationally symmetric case. Imagine two open cylinders, the smaller nested inside the larger. Next fill the trough between the two cylinders with a viscious fluid - silicon oil is a good example. The spreading that we are modeling occurs when the smaller cylinder vanishes, causing the fluid to flow into the center. Particularly interesting is what happens at the moment the fluid converges and focuses at the center.
These are movies of two stages of the rotationally symmetric case:
The Beginning (400K)
What you are seeing is a cut-away view showing only half of the ring of
liquid. To illustrate the sinking of the liquid as it flows, the central
cylinder has been replaced by a more conical dam. When you hit play, this
support is removed and the fluid pours inward.
Focusing (300K)
Here the liquid spreads completely over the floor and then rises to fill the
container.
The second case is a non-symmetric one. Particularly interesting are any symmetries that might occur as the focusing moment is reached.
A.L. Bertozzi, M.P. Brenner, T.F. Dupont, and L.P. Kadanoff, Singularites and similariteis in interface flow, in "Trends and Perspectives in Applied Mathematics", (L. Sirovich, editor), Springer-Verlag, 1994.
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Created: June 2 1995 ---
Last modified: Jun 18 1996