Centrifugal instability of Taylor-Couette flow in stratified and diffusive fluids
arXiv:2512.08664 · doi:10.1017/jfm.2025.261
Abstract
The linear and non-linear dynamics of centrifugal instability in Taylor-Couette flow are investigated when fluids are stably stratified and highly diffusive. One-dimensional local linear stability analysis (LSA) on cylindrical Couette flow confirms that the stabilising role of stratification on centrifugal instability is suppressed by strong thermal diffusion (i.e. low Prandtl number ). For , it is verified that the instability dependence on thermal diffusion and stratification with the non-dimensional Brunt-Väisälä frequency can be prescribed by a single rescaled parameter . From direct numerical simulation (DNS), various non-linear features such as axisymmetric Taylor vortices at saturation, secondary instability leading to non-axisymmetric patterns or transition to chaotic states are investigated for various values of and the Reynolds number . Two-dimensional bi-global LSA on axisymmetric Taylor vortices, which appear as primary centrifugal instability saturates nonlinearly, is also performed to find the secondary critical Reynolds number at which the Taylor vortices become unstable by non-axisymmetric perturbation. The bi-global LSA reveals that increases (i.e. the onset of secondary instability is delayed) in the range at or as increases at . Secondary instability leading to highly non-axisymmetric or irregular chaotic patterns is further investigated by the 3D DNS. The Nusselt number is also computed from the torque at the inner cylinder for various and at to describe how the angular momentum transfer increases with and how varies differently for saturated and chaotic states.
arXiv commentaccepted manuscript in Journal of Fluid Mecahnics
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