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On the artificial compressibility method for the Navier-Stokes-Fourier system

Donatella Donatelli
- 21 May 2010 - 
- Vol. 68, Iss: 3, pp 469-485
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TLDR
In this paper, the authors deal with the artificial compressibility approximation method adapted to the incompressible Navier Stokes Fourier system, and two different types of approximations are analyzed: one for the full NSF system where viscous heating effects are considered and the other for when the dissipative function S: ∇u is omitted.
Abstract
This paper deals with the artificial compressibility approximation method adapted to the incompressible Navier Stokes Fourier system. Two different types of approximations will be analyzed: one for the full Navier Stokes Fourier system (or the so-called Rayleigh-Benard equations) where viscous heating effects are considered and the other for when the dissipative function S: ∇u is omitted. The convergence of the approximating sequences is achieved by exploiting the dispersive properties of the wave equation structure of the pressure of the approximating system.

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Journal ArticleDOI

Leray weak solutions of the incompressible Navier Stokes system on exterior domains via the artificial compressibility method

TL;DR: In this paper, the Leray weak solutions of the incompressible Navier Stokes equation in an exterior domain were studied and the strong convergence analysis of the velocity field was achieved by using the associated Leray-Hodge decomposition.
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The artificial compressibility approximation for mhd equations in unbounded domain

TL;DR: In this paper, a method of approximation for the weak solutions of the incompressible magnetohydrodynamic equations (MHD) in unbounded domains is presented. But the method is not suitable for the case of weak MHD.
Journal ArticleDOI

On the spectrum for the artificial compressible system

TL;DR: It is proved that if a stationary solution of the incompressible system is asymptotically stable and the velocity field of the stationary solution satisfies an energy-type stability criterion by variational method, then it is also stable as a solutions of the artificial compressible one for sufficiently small ϵ.
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Stability of Bifurcating Stationary Solutions of the Artificial Compressible System

TL;DR: It is proved that when a stationary bifurcation from a simple eigenvalue occurs, the range of $$\epsilon $$ϵ can be taken uniformly near the b ifurcation point to conclude the stability of the bIfurcating solution as a solution of the artificial compressible system.
Journal ArticleDOI

An interpretation of Temam’s extra force in the quasi-incompressible Navier–Stokes system

TL;DR: In this article, the role of the extra force density f e = − 1 2 ( ∇ · v ) v in the adimensionalized system of partial differential equations is discussed.
References
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Book

Harmonic Analysis: Real-variable Methods, Orthogonality, and Oscillatory Integrals

TL;DR: In this article, the authors introduce the Heisenberg group and describe the Maximal Operators and Maximal Averages and Oscillatory Integral Integrals of the First and Second Kind.
Journal ArticleDOI

Numerical solution of the Navier-Stokes equations

TL;DR: In this paper, a finite-difference method for solving the time-dependent Navier-Stokes equations for an incompressible fluid is introduced, which is equally applicable to problems in two and three space dimensions.
Book

Navier-Stokes Equations

Roger Temam
TL;DR: Schiff's base dichloroacetamides having the formula OR2 PARALLEL HCCl2-C-N ANGLE R1 in which R1 is selected from the group consisting of alkenyl, alkyl, alkynyl and alkoxyalkyl; and R2 is selected by selecting R2 from the groups consisting of lower alkylimino, cyclohexenyl-1 and lower alkynyl substituted cycloenenyl -1 as discussed by the authors.
Journal ArticleDOI

Compact sets in the spaceL p (O,T; B)

TL;DR: In this paper, a characterization of compact sets in Lp (0, T; B) is given, where 1⩽P⩾∞ and B is a Banach space.
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