Abstract:Abstract. We consider the mild solutions of the Prandtl equations on the half space. Requiring analyticity only with respect to the tangential variable, we prove the short time existence and the uniqueness of the solution in the proper function space. The proof is achieved applying the abstract Cauchy-Kowalewski theorem to the boundary layer equations once the convection-diffusion operator is explicitly inverted. This improves the result of [M. Sammartino and R. E. Caflisch, Comm. Math. Phys., 192 (1998), pp.… Show more
“…Thus the solvability of the Prandtl equations itself is not surprising in our setting; cf. [2,32,17]. But we note here that the solvability of the Prandtl equations does not necessarily imply the desired asymptotic expansion, as in the counter example by [10].…”
Section: The Spaceẇmentioning
confidence: 80%
“…The analyticity condition is in fact required only in the tangential direction [17]. But the solvability for general initial data in a Sobolev class is still an open problem.…”
We consider the Navier-Stokes equations for viscous incompressible flows in the half plane under the no-slip boundary condition. By using the vorticity formulation we prove the (local in time) convergence of the Navier-Stokes flows to the Euler flows outside a boundary layer and to the Prandtl flows in the boundary layer at the inviscid limit when the initial vorticity is located away from the boundary.
“…Thus the solvability of the Prandtl equations itself is not surprising in our setting; cf. [2,32,17]. But we note here that the solvability of the Prandtl equations does not necessarily imply the desired asymptotic expansion, as in the counter example by [10].…”
Section: The Spaceẇmentioning
confidence: 80%
“…The analyticity condition is in fact required only in the tangential direction [17]. But the solvability for general initial data in a Sobolev class is still an open problem.…”
We consider the Navier-Stokes equations for viscous incompressible flows in the half plane under the no-slip boundary condition. By using the vorticity formulation we prove the (local in time) convergence of the Navier-Stokes flows to the Euler flows outside a boundary layer and to the Prandtl flows in the boundary layer at the inviscid limit when the initial vorticity is located away from the boundary.
“…[7,[15][16][17][18]28,41]), we use the following version of the Abstract CauchyKowalevski Theorem (ACK) (cf. [1,35,47] and references therein). Consider the equation u + F(u, t) = 0.…”
The aim of this paper is to prove that the solutions of the primitive equations converge, in the zero viscosity limit, to the solutions of the hydrostatic Euler equations. We construct the solution of the primitive equations through a matched asymptotic expansion involving the solution of the hydrostatic Euler equation and boundary layer correctors as the first order term, and an error that we show to be O( √ ν). The main assumption is spatial analyticity of the initial datum.
“…One brief remark here is that the Prandtl equations are well posed only under strong conditions on the flow, such as when boundary and the data have some degree of analyticity [5,128,95,23,84] or the data is monotonic in the normal direction to the boundary [122,124,83]. The most classical result verifying (3.9) is [128] in the analytic functional framework, after the pioneering work of [5,6].…”
Section: Case Of No-slip Boundary Conditionmentioning
The validity of the vanishing viscosity limit, that is, whether solutions of the Navier-Stokes equations modeling viscous incompressible flows converge to solutions of the Euler equations modeling inviscid incompressible flows as viscosity approaches zero, is one of the most fundamental issues in mathematical fluid mechanics. The problem is classified into two categories: the case when the physical boundary is absent, and the case when the physical boundary is present and the effect of the boundary layer becomes significant. The aim of this article is to review recent progress on the mathematical analysis of this problem in each category.
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