In this paper, we consider the Navier Stokes equations for isentropic, compressible flows of a polytropic gas in a bounded domain. The equations to be considered are obtained by scaling to dimensionless form and then replacing the density \ by \Ä += 2 \, where = is a Mach number. The existence of so
Steady compressible Navier–Stokes equations with large potential forces via a method of decomposition
✍ Scribed by Antonin Novotny; Konstantin Pileckas
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 158 KB
- Volume
- 21
- Category
- Article
- ISSN
- 0170-4214
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✦ Synopsis
Communicated by Y. Shibata
We investigate the steady compressible Navier-Stokes equations near the equilibrium state v"0, " (v the velocity, the density) corresponding to a large potential force. We introduce a method of decomposition for such equations: the velocity field v is split into a non-homogeneous incompressible part u (div ( u)"0) and a compressible (irrotational) part . In such a way, the original complicated mixed elliptic-hyperbolic system is split into several 'standard' equations: a Stokes-type system for u, a Poisson-type equation for and a transport equation for the perturbation of the density " ! . For "const. (zero potential forces), the method coincides with the decomposition of Novotny and Padula [21]. To underline the advantages of the present approach, we give, as an example, a 'simple' proof of the existence of isothermal flows in bounded domains with no-slip boundary conditions. The approach is applicable, with some modifications, to more complicated geometries and to more complicated boundary conditions as we will show in forthcoming papers.
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