paper

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)

Cited by in corpus (5)