Global-in- Stability of Steady Prandtl Expansions for 2D Navier-Stokes Flows
arXiv:2008.12347
Abstract
In this work, we establish the convergence of 2D, stationary Navier-Stokes flows, to the classical Prandtl boundary layer, , posed on the domain : \begin{equation*} \| u^ε - \bar{u}_p \|_{L^\infty_y} \lesssim \sqrtε \langle x \rangle^{- \frac 1 4 + δ}, \qquad \| v^ε - \sqrtε \bar{v}_p \|_{L^\infty_y} \lesssim \sqrtε \langle x \rangle^{- \frac 1 2}. \end{equation*} This validates Prandtl's boundary layer theory \textit{globally} in the -variable for a large class of boundary layers, including the entire one parameter family of the classical Blasius profiles, with sharp decay rates. The result demonstrates asymptotic stability in two senses simultaneously: (1) asymptotic as and (2) asymptotic as . In particular, our result provides the first rigorous confirmation for the Navier-Stokes equations that the boundary layer cannot "separate" in these stable regimes, which is very important for physical and engineering applications.
73 pages. Submitted
References in corpus (6)
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Cited by in corpus (5)
- Boundary Layer Expansions for the Stationary Navier-Stokes Equations
- Remarks on the Steady Prandtl Boundary Layer Expansions
- Global-in- stability of Prandtl layer expansions for steady magnetohydrodynamics flows over a moving plate
- Validity of Prandtl layer theory for steady magnetohydrodynamics over a moving plate with nonshear outer ideal MHD flows
- Asymptotic Behavior of the Steady Prandtl Equation