Zero Viscosity Limit for Analytic Solutions of the Navier-Stokes Equation on a Half-Space.¶ II. Construction of the Navier-Stokes Solution

Sammartino, M.; Caflisch, Russel E.

doi:10.1007/s002200050305

Cited by 335 publications

(258 citation statements)

References 8 publications

Supporting

Mentioning

245

Contrasting

Unclassified

Order By: Relevance

“…In fact we show that the time of existence of a regular solution does not depend on the boundary layer solution whereas in [4] and [5] the size of the domain of analyticity was shrinking at each step of the asymptotic expansion.…”

mentioning

confidence: 80%

See 1 more Smart Citation

Analytic solutions of the Navier-Stokes equations

Lombardo

2001

Rend. Circ. Mat. Palermo

View full text Add to dashboard Cite

show abstract

mentioning

confidence: 80%

“…Our analysis will strictly follow Sammartino and Caflish ( [4] and [5]). In their papers the authors proved that the solution of the Navier-Stokes equations with analytic initial data can be decomposed in the form of an asymptotic series.…”

mentioning

confidence: 99%

Analytic solutions of the Navier-Stokes equations

Lombardo

2001

Rend. Circ. Mat. Palermo

View full text Add to dashboard Cite

show abstract

“…k f is the kth Fourier coefficient of the operator which inverts the heat equation with homogeneous boundary and initial data, E (1) k g is the kth Fourier coefficient of the operator which solves the homogeneous heat equation with nonzero boundary data and zero initial data and E (0) k u 0 is the kth Fourier coefficient of the operator which solves the homogeneous heat equation with zero boundary data and nonzero initial data.…”

Section: In the Above Expressions E (2)mentioning

confidence: 99%

“…In [1] it was proved that, for analytic solutions of the Navier-Stokes equations on the half space and for a short time, these approximations are indeed…”

Section: Introductionmentioning

confidence: 99%

Asymptotic Analysis of the Linearized Navier–stokes Equation on an Exterior Circular Domain: Explicit Solution and the Zero Viscosity Limit

Lombardo

Caflisch

Sammartino

2001

Communications in Partial Differential Equations

Self Cite

View full text Add to dashboard Cite

In this paper we study and derive explicit formulas for the linearized Navier-Stokes equations on an exterior circular domain in space dimension two. Through an explicit construction, the solution is decomposed into an inviscid solution, a boundary layer solution and a corrector. Bounds on these solutions are given, in the appropriate Sobolev spaces, in terms of the norms of the initial and boundary data. The correction term is shown to be of the same order of magnitude as the square root of the viscosity.

show abstract

“…The stationary Prandtl system has been widely studied [12]. Despite its importance in engeneering applications [7], [15], very few results are known for the existence of (global in time) solutions of the instationary system [12,13,14]. In both cases, the stationary and the instationary one, a possible way to tackle the problem consists in using the so-called Crocco transformation [12].…”

Section: Introductionmentioning

confidence: 99%

The Linearized Crocco Equation

Buchot

Raymond

2006

J. math. fluid mech.

View full text Add to dashboard Cite

Abstract. In this paper, we study the existence and uniqueness of a degenerate parabolic equation, with nonhomogeneous boundary conditions, coming from the linearization of the Crocco equation [12]. The Crocco equation is a nonlinear degenerate parabolic equation obtained from the Prandtl equations with the so-called Crocco transformation. The linearized Crocco equation plays a major role in stabilization problems of fluid flows described by the Prandtl equations [5]. To study the infinitesimal generator associated with the adjoint linearized Crocco equation -with homogeneous boundary conditions -we first study degenerate parabolic equations in which the x-variable plays the role of a time variable. This equation is doubly degenerate: the coefficient in front of ∂x vanishes on a part of the boundary, and the coefficient of the elliptic operator vanishes in another part of the boundary. This makes very delicate the proof of uniqueness of solution. To overcome this difficulty, a uniqueness result is first obtained for an equation in which the elliptic operator is symmetric, and it is next extended to the original equation by combining an iterative process and a fixed point argument (see Th. 4.9). This kind of argument is also used to prove estimates, which cannot be obtained in a classical way. Mathematics Subject Classification (2000). Primary 35K65 ; Secondary 35Q35, 76D10.

show abstract

Zero Viscosity Limit for Analytic Solutions of the Navier-Stokes Equation on a Half-Space.¶ II. Construction of the Navier-Stokes Solution

Cited by 335 publications

References 8 publications

Analytic solutions of the Navier-Stokes equations

Analytic solutions of the Navier-Stokes equations

Asymptotic Analysis of the Linearized Navier–stokes Equation on an Exterior Circular Domain: Explicit Solution and the Zero Viscosity Limit

The Linearized Crocco Equation

Contact Info

Product

Resources

About