Zero viscosity and thermal diffusivity limit of the linearized compressible Navier–Stokes–Fourier equations in the half plane

Article type: Research Article

Authors: Ding, Yutao^a | Jiang, Ning^{b; *}

Affiliations: [a] Mathematical Sciences Center, Jin Chunyuan West Building, Beijing, 100084, P.R. China. E-mail: [email protected] | [b] School of Mathematics and Statistics, Wuhan University, Wuhan, 430072, P.R. China. E-mail: [email protected]

Correspondence: [*] Corresponding author. E-mail: [email protected].

Abstract: We study the zero viscosity and thermal diffusivity limit of an initial boundary problem for the linearized Navier–Stokes–Fourier equations of a compressible viscous and heat conducting fluid in the half plane. We consider the case that the viscosity and thermal diffusivity converge to zero at the same order. The approximate solution of the linearized Navier–Stokes–Fourier equations with inner and boundary expansion terms is analyzed formally first by multiscale analysis. Then the pointwise estimates of the error terms of the approximate solution are obtained by energy methods. Thus establish the uniform stability for the linearized Navier–Stokes–Fourier equations in the zero viscosity and heat conductivity limit. This work is based on (Comm. Pure Appl. Math. 52 (1999), 479–541) and generalize their results from isentropic case to the general compressible fluid with thermal diffusive effect. Besides the viscous layer as in (Comm. Pure Appl. Math. 52 (1999), 479–541), the thermal layer appears and couples with the viscous layer linearly.

Keywords: Compressible Navier–Stokes, Prandtl equations, boundary layer, thermal diffusivity, zero viscosity

DOI: 10.3233/ASY-211673

Journal: Asymptotic Analysis, vol. 127, no. 1-2, pp. 57-96, 2022