Low Mach number Limit of Steady Thermally Driven Fluid

Fuente: arXiv
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Auteurs principaux: Huang, Feimin, Wang, Weiqiang, Wang, Yong
Format: Preprint
Publié: 2024
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author Huang, Feimin
Wang, Weiqiang
Wang, Yong
author_facet Huang, Feimin
Wang, Weiqiang
Wang, Yong
contents In this paper, we establish the existence of strong solutions to the steady non-isentropic compressible Navier-Stokes system with Dirichlet boundary conditions in bounded domains where the fluid is driven by the wall temperature, and justify its low Mach number limit, i.e., $\v\to 0$, in $L^{\infty}$ sense with a rate of convergence. Notably, for the limiting system \eqref{fge} obtained in the low Mach number limit, the variation of the wall temperature is allowed to be independent of the Mach number. It is also worth pointing out that the velocity field $u_{1}$ acts like a ghost since it appears at $\v$-order in the expansion, but still affects the density and temperature at $O(1)$-order. In the proof, we design a new expansion, in which the density, velocity and temperature have different expansion forms with respect to $\v$, so that the density at higher orders is well-defined under the Boussinesq relations and the constraint of zero average. We also introduce a new $\v$-dependent functional space, allowing us to obtain some uniform estimates for high-order normal derivatives near the boundary.
format Preprint
id arxiv_https___arxiv_org_abs_2407_16400
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Low Mach number Limit of Steady Thermally Driven Fluid
Huang, Feimin
Wang, Weiqiang
Wang, Yong
Analysis of PDEs
In this paper, we establish the existence of strong solutions to the steady non-isentropic compressible Navier-Stokes system with Dirichlet boundary conditions in bounded domains where the fluid is driven by the wall temperature, and justify its low Mach number limit, i.e., $\v\to 0$, in $L^{\infty}$ sense with a rate of convergence. Notably, for the limiting system \eqref{fge} obtained in the low Mach number limit, the variation of the wall temperature is allowed to be independent of the Mach number. It is also worth pointing out that the velocity field $u_{1}$ acts like a ghost since it appears at $\v$-order in the expansion, but still affects the density and temperature at $O(1)$-order. In the proof, we design a new expansion, in which the density, velocity and temperature have different expansion forms with respect to $\v$, so that the density at higher orders is well-defined under the Boussinesq relations and the constraint of zero average. We also introduce a new $\v$-dependent functional space, allowing us to obtain some uniform estimates for high-order normal derivatives near the boundary.
title Low Mach number Limit of Steady Thermally Driven Fluid
topic Analysis of PDEs
url https://arxiv.org/abs/2407.16400