Non-axisymmetric rotating-disk flows: nonlinear travelling-wave states

Citation
Re. Hewitt et Pw. Duck, Non-axisymmetric rotating-disk flows: nonlinear travelling-wave states, J FLUID MEC, 413, 2000, pp. 287-316
Citations number
16
Categorie Soggetti
Physics,"Mechanical Engineering
Journal title
JOURNAL OF FLUID MECHANICS
ISSN journal
00221120 → ACNP
Volume
413
Year of publication
2000
Pages
287 - 316
Database
ISI
SICI code
0022-1120(20000625)413:<287:NRFNTS>2.0.ZU;2-M
Abstract
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.