Abstract
A thin annular layer of fluid coating a cylinder is subject to two different instabilities. One, driven by surface tension, is analogous to the Rayleigh instability of a liquid jet. The other is the Rayleigh–Taylor instability, which is driven by gravity. Measurements of the wavelength and growth rate of periodic patterns of droplets which develop as a result of the instability of such a fluid layer are reported for cylinders with radius r in the range 0.0011<r<1.27 cm. For small r the wavelength and growth rate of the pattern are in agreement with theoretical predictions for the surface-tension-driven instability. For large r, the Rayleigh–Taylor instability is observed. At intermediate r there is a region of crossover between the two limiting cases.