OK. Polyester films are coated for many applications, running in long continuous strips, 0.005" thick, 12" wide, 1000s ft long (give or take an order of magnitude on each). The film is run through a series of "rollers", with the wrap angle on a given roller of 10 to 180 degrees depending on the "web path" moving from roller 1 to 2 to 3 and so on. These rollers support the web in the curved shape.
The moving web is controlled to run at a given speed, but also a machine direction tension, typically 1 lbf per in of width. This tension pulled over the cylindrical roller creates a pressure on the cylinder of Tension/Width/Radius (psi).
In some cases, to it is desirable not to contact the center of the web (it is contact sensitive to scratching or contamination). In these cases, an undercut roller, a cylinder with small diameter in the center, is used, so the curved, tensioned film is only supported at the two ends. The problem is understanding what conditions this is unstable, where the cylinder created by the polyester film will buckle rather that hold its cylindrical shape. Radius, unsupported width, tension, modulus, thickness, supported width, all seem to be factors.
This doesn't fit Euler's buckling criteria, since it is not axially loaded. Also, the slenderness ratio (L/r) places most cases in the "short column" catagory. Lastly, an axial loading model will show larger diameters support more load, where I know from practice, that small diameters are stiffer for this scenario.
Does this give you a better picture?