Abstract
In this article, we prove that the threshold of instability of the classical Couette flow in Hs for large s is ν1/2. The instability is completely driven by the boundary. The dynamic of the flow creates a Prandtl type boundary layer of width ν1/2 which is itself linearly unstable. This leads to a secondary instability which in turn creates a sub-layer.
| Original language | English | 
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| Article number | 221 | 
| Journal | Communications in Mathematical Physics | 
| Volume | 406 | 
| Issue number | 9 | 
| DOIs | |
| Publication status | Published - Sept 2025 |