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The three-dimensional linear instability of axisymmetric flow between exactly counter-rotating disks is studied numerically. The dynamics are governed by two parameters, the Reynolds number $Re$ based on cylinder radius and disk rotation speed and the height-to-radius ratio Γ . The stability analysis performed for 0.5 \,≤\, Γ \,≤\, 3 shows that non-axisymmetric modes are dominant and stationary and that the critical azimuthal wavenumber is a decreasing function of Γ . The patterns of the dominant perturbations are analysed and a physical mechanism related to a shear layer instability is discussed. No evidence of complex dynamical behaviour is seen in the neighbourhood of the 1:2 codimension-two point when the m\,=\,2 threshold precedes that of m\,=\,1 . Axisymmetric instabilities are also calculated; these may be stationary or Hopf bifurcations. Their thresholds are always higher than those of non-axisymmetric modes.
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Nore et al. (2004) studied this question.
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