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Members of this team are all working on problems involving capillary surfaces. The mathematical
and physical background necessary for all subprojects is essentially the same.
Please list any and all references that you find useful here.
For image processing you have several choices. MATLAB has a built in image processing toolbox.
MATLAB is available on the computers in the lab. You might also try the program ImageJ. This is
free program developed by the NIH. The link is to a Windows version. It is fairly sophisticated in
its abilities, yet easy to use.
A long cylindrical column of fluid is unstable to spatial perturbations. You can observe this easily
in your kitchen by turning on your faucet so that only a small stream of water comes out. Notice
that the column breaks up into droplets by the time it reaches the bottom of your sink. Mathematical
approaches to understanding this instability are essential to master for all of the capillary projects we are
undertaking. We'll discuss this instability in more detail in group meetings. The following picture
will be the focus of our discussion. Click Rayleigh-Plateau for a more detailed page on this instability.

If you insert a capillary tube into a fluid, the fluid will rise in the tube to a height higher than the surrounding
liquid. This is a classic, long studied problem, but we need to understand this in order to do the dynamic problem.
Anson Carter has worked through this problem and presented his results in group meetings. The results can
be found Here.
In this project we study the motion of flexible bodies driven by the capillary force. The classic example of capillary
driven motion is the so-called "Cheerio's Effect." We want to understand this effect and then extend the analysis to
the case of bodies that can deform. The information can be obtained on this page.
In this project we study the dynamic motion of fluid surfaces driven by capillary forces. We look at the rise of fluid in
a capillary tube and the rise of fluid in a wedge. The detailed page on this is here.
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