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Transition threshold for the 2-D Couette flow in a finite channel
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abstract
In this paper, we study the transition threshold problem for the 2-D Navier-Stokes equations around the Couette flow $(y,0)$ at large Reynolds number $Re$ in a finite channel. We develop a systematic method to establish the resolvent estimates of the linearized operator and space-time estimates of the linearized Navier-Stokes equations. In particular, three kinds of important effects: enhanced dissipation, inviscid damping and boundary layer, are integrated into the space-time estimates in a sharp form. As an application, we prove that if the initial velocity $v_0$ satisfies $\|v_0-(y, 0)\|_{H^2}\le cRe^{-\frac 12}$ for some small $c$ independent of $Re$, then the solution of the 2-D Navier-Stokes equations remains within $O(Re^{-\frac 12})$ of the Couette flow for any time.
Forward citations
Cited by 3 Pith papers
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Stability threshold of the 2D Couette flow in Sobolev spaces
For 2D Navier-Stokes near Couette flow, H^σ vorticity perturbations of size ≤ ε Re^{-1/3} are globally stable with inviscid damping and enhanced dissipation.
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Enhanced dissipation for the 2D Couette flow in critical space
For 2D Navier-Stokes near Couette, ν^{1/2}-small perturbations in H^log_x L^2_y undergo enhanced dissipation at rate ν^{1/3} and inviscid damping, with L^2 initial data sufficient for any threshold exponent above 1/2.
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On the stability of laminar flows between plates
Monotone shear flows that are either nearly linear or have no inflection point are linearly stable in the large Reynolds limit, in a periodic channel with no-slip or traction boundary conditions.
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