We consider the classical problem of the laminar flow of an incompressible
rotating fluid above a rotating, impermeable, infinite disk. There is a wel
l-known class of solutions to this configuration in the form of an exact ax
isymmetric solution to the Navier-Stokes equations. However, the radial sel
f-similarity that leads to the 'rotating disk equations' can also be used t
o obtain solutions that are non-axisymmetric in nature, although (in genera
l) this requires a boundary-layer approximation. In this manner, we locate
several new solution branches, which are non-axisymmetric travelling-wave s
tates that satisfy axisymmetric boundary conditions at infinity and at the
disk. These states are shown to appear as symmetry-breaking bifurcations of
the well-known axisymmetric solution branches of the rotating-disk equatio
ns. Numerical results are presented, which suggest that an infinity of such
travelling states exist in some parameter regimes. The numerical results a
re also presented in a manner that allows their application to the analogou
s flow in a conical geometry.
Two of the many states described are of particular interest. The first is a
n exact, nonlinear, non-axisymmetric, stationary state for a rotating disk
in a counter-rotating fluid; this solution was first presented by Hewitt, D
uck & Foster (1999) and here we provide further details. The second state c
orresponds to a new boundary-layer-type approximation to the Navier-Stokes
equations in the form of azimuthally propagating waves in a rotating fluid
above a stationary disk. This second state is a new nonaxisymmetric alterna
tive to the classical axisymmetric Bodewadt solution.