Knudsen boundary layer equations with incoming boundary condition: full range of cutoff collision kernels and Mach numbers of the far field

Fuente: arXiv
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Autori principali: Jiang, Ning, Luo, Yi-Long, Wu, Yulong, Yang, Tong
Natura: Preprint
Pubblicazione: 2025
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author Jiang, Ning
Luo, Yi-Long
Wu, Yulong
Yang, Tong
author_facet Jiang, Ning
Luo, Yi-Long
Wu, Yulong
Yang, Tong
contents This paper establishes tahe existence and uniqueness of the nonlinear Knudsen layer equation with incoming boundary conditions. It is well-known that the solvability conditions of the problem vary with the Mach number of the far Maxwellian $\mathcal{M}^\infty$. We consider full ranges of cutoff collision kernels (i.e., $- 3 < γ\leq 1$) and all the Mach numbers of the far field in the $L^\infty_{x,v}$ framework. Additionally, the solution exhibits exponential decay $\exp \{- c x^\frac{2}{3 - γ} - c |v|^2 \}$ for some $c > 0$. To address the general angular cutoff collision kernel, we introduce a $(x,v)$-mixed weight $σ$. The proof is essentially bsed on adding an artificial damping term.
format Preprint
id arxiv_https___arxiv_org_abs_2501_04035
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Knudsen boundary layer equations with incoming boundary condition: full range of cutoff collision kernels and Mach numbers of the far field
Jiang, Ning
Luo, Yi-Long
Wu, Yulong
Yang, Tong
Analysis of PDEs
35Q20, 76P05, 35F30, 35B45, 35A01, 35A02
This paper establishes tahe existence and uniqueness of the nonlinear Knudsen layer equation with incoming boundary conditions. It is well-known that the solvability conditions of the problem vary with the Mach number of the far Maxwellian $\mathcal{M}^\infty$. We consider full ranges of cutoff collision kernels (i.e., $- 3 < γ\leq 1$) and all the Mach numbers of the far field in the $L^\infty_{x,v}$ framework. Additionally, the solution exhibits exponential decay $\exp \{- c x^\frac{2}{3 - γ} - c |v|^2 \}$ for some $c > 0$. To address the general angular cutoff collision kernel, we introduce a $(x,v)$-mixed weight $σ$. The proof is essentially bsed on adding an artificial damping term.
title Knudsen boundary layer equations with incoming boundary condition: full range of cutoff collision kernels and Mach numbers of the far field
topic Analysis of PDEs
35Q20, 76P05, 35F30, 35B45, 35A01, 35A02
url https://arxiv.org/abs/2501.04035