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The Sobolev Stability Threshold for 2D Shear Flows Near Couette
The Sobolev Stability Threshold for 2D Shear Flows Near Couette
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The Sobolev Stability Threshold for 2D Shear Flows Near Couette
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The Sobolev Stability Threshold for 2D Shear Flows Near Couette
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The Sobolev Stability Threshold for 2D Shear Flows Near Couette
The Sobolev Stability Threshold for 2D Shear Flows Near Couette
Journal Article

The Sobolev Stability Threshold for 2D Shear Flows Near Couette

2018
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Overview
We consider the 2D Navier–Stokes equation on T × R , with initial datum that is ε -close in H N to a shear flow ( U ( y ), 0), where ‖ U ( y ) - y ‖ H N + 4 ≪ 1 and N > 1 . We prove that if ε ≪ ν 1 / 2 , where ν denotes the inverse Reynolds number, then the solution of the Navier–Stokes equation remains ε -close in H 1 to ( e t ν ∂ y y U ( y ) , 0 ) for all t > 0 . Moreover, the solution converges to a decaying shear flow for times t ≫ ν - 1 / 3 by a mixing-enhanced dissipation effect, and experiences a transient growth of gradients. In particular, this shows that the stability threshold in finite regularity scales no worse than ν 1 / 2 for 2D shear flows close to the Couette flow.