Abstract
In this survey, we study the boundary value problem for the stationary Navier–Stokes system in planar exterior domains. With no-slip boundary condition and a prescribed constant limit velocity at infinity, this problem describes stationary Navier–Stokes flows around cylindrical obstacles. Leray’s invading domains method is presented as a starting point. Then we discuss the boundedness and convergence of general D-solutions (solutions with finite Dirichlet integrals) in exterior domains. For the Leray solutions of the flow around an obstacle problem, we study the nontriviality, and the justification of the limit velocity at small Reynolds numbers. Further, under the same assumption of small Reynolds numbers the global uniqueness theorem for the problem is established in the class of D-solutions, its proof deals with the accurate perturbative analysis based on the linear Oseen system, inspired by classical Finn-Smith technique; the classical Amick and Gilbarg–Weinberger papers are involved here as well. The forced Navier–Stokes system in the whole plane is also presented as a closely related problem. A list of unsolved problems is given at the end of the paper.
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Notes
Stokes himself gave the following explanation: The pressure of the cylinder on the fluid continuously tends to increase the quantity of fluid which it carries with it, while the friction of the fluid at a distance from the cylinder continually tends to diminish it. In the case of a sphere, these two causes eventually counteract each other, and the motion becomes uniform. But in the case of a cylinder, the increase in the quantity of the fluid carried continually gains on the decrease due to the friction of the surrounding fluid, and the quantity carried increases indefinitely as the cylinder moves on [37, p. 65].
This convergence is uniform on every bounded set.
It is natural to restrict our attention to the class of D-solutions since the Dirichlet integral is the natural energy integral for the stationary Navier–Stokes system. Physically, finiteness of the Dirichlet integral means that the total energy dissipation rate in the fluid is finite.
The irony of fate—precisely because of the embedding theorems, the Millennium problem for the dynamical NS-system is easily solved in the two-dimensional case, and remains unapproachable for the three-dimensional case.
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In honor of Professor Olga Ladyzhenskaya. This article is part of the Topical collection Ladyzhenskaya Centennial Anniversary edited by Gregory Seregin, Konstantinas Pileckas and Lev Kapitanski.
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Korobkov, M., Ren, X. Stationary Solutions to the Navier–Stokes System in an Exterior Plane Domain: 90 Years of Search, Mysteries and Insights. J. Math. Fluid Mech. 25, 55 (2023). https://doi.org/10.1007/s00021-023-00792-w
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DOI: https://doi.org/10.1007/s00021-023-00792-w