Abstract
Since THE Early Work of Taylor (I)†, it has become well known that the Couette flow between an inner, rotating circular cylinder and a concentric, stationary outer cylinder becomes unstable at sufficiently high rotational speeds. The initial instability leads to the formation of a series of toroidal vortices, commonly referred to as Taylor vortices. The vortices occupy approximately square cells, and adjacent pairs are contra-rotating. When the gap d between the cylinders is small compared with the inner cylinder radius R1, the criterion for the onset on the instability is the Taylor number T = Ω1R1d3 / v2 where Ω1 is the rotational speed and v the kinematic viscosity of the fluid. A widely accepted critical value is Tc = 1708. Recently Coles (2) has shown the existence of a second instability consisting of travelling circumferential waves superimposed on the Taylor vortices.
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