Abstract
The stability of a pulsed flow in a Taylor-Couette geometry with both cylinders rotating at the same angular velocity Ω(t) = Ω0 cos(ωt) is investigated. The first experimental evidence showing that the flow is less unstable in the limit of low and high frequency while destabilization is maximum for an intermediate frequency ω0 is reported. A detailed analysis of the restabilization at frequencies just above ω0 reveals a behavior not accounted for by previous theoretical analysis. Thus, the linear stability analysis is reconsidered by using a different implementation of the Floquet theory and a satisfactory agreement with the present experimental results is found.
| Original language | English |
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| Pages (from-to) | 3665-3676 |
| Number of pages | 12 |
| Journal | Physics of Fluids |
| Volume | 6 |
| Issue number | 11 |
| DOIs | |
| Publication status | Published - 1 Jan 1994 |
| Externally published | Yes |