Rayleigh-Taylor instability of an inclined buoyant viscous cylinder

The Rayleigh-Taylor instability of an inclined buoyant cylinder of one very viscous fluid rising through another is examined through linear stability analysis, numerical simulation and experiment. The stability analysis represents linear eigenmodes of a given axial wavenumber as a Fourier series in the azimuthal direction, allowing the use of separable solutions to the Stokes equations in cylindrical polar coordinates. The most unstable wavenumber k(*) is long-wave if both the inclination angle alpha and the viscosity ratio lambda (internal/external) are small; for this case, k* proportional to max{alpha, (lambda ln lambda(-1))(1/2)} and thus a small angle in experiments can have a significant effect for lambda << 1. As alpha increases, the maximum growth rate decreases and the upward propagation rate of disturbances increases; all disturbances propagate without growth if the cylinder is sufficiently close to vertical, estimated as alpha greater than or similar to 70 degrees. Results from the linear stability analysis agree with numerical calculations for lambda = 1 and experimental observations. A point-force numerical method is used to calculate the development of instability into a chain of individual plumes via a complex three-dimensional flow. Towed-source experiments show that nonlinear interactions between neighbouring plumes are important for alpha greater than or similar to 20 degrees and that disturbances can propagate out of the system without significant growth for alpha greater than or similar to 40 degrees.