Linear Half-Space Problems in Kinetic Theory: Abstract Formulation and Regime Transitions

TL;DR

This paper formulates a general half-space problem in kinetic theory, investigates conditions for well-posedness, and analyzes regime transitions between evaporation and condensation, revealing how to achieve uniform exponential convergence.

Contribution

It introduces a generalized formulation of kinetic half-space problems and studies regime transitions, providing conditions to ensure uniform exponential decay near these transitions.

Findings

Exponential convergence away from the interface

Conditions for well-posedness depend on the interface data

Elimination of slowly varying modes near regime transitions

Abstract

Half-space problems in the kinetic theory of gases are of great importance in the study of the asymptotic behavior of solutions of boundary value problems for the Boltzmann equation for small Knudsen numbers. In this work a generally formulated half-space problem, based on generalizations of stationary half-space problems in one spatial variable for the Boltzmann equation - for hard-sphere models of monatomic single species and multicomponent mixtures - is considered. The number of conditions on the indata at the interface needed to obtain well-posedness is investigated. Exponential fast convergence is obtained "far away" from the interface. In particular, the exponential decay at regime transitions - where the number of conditions on the indata needed to obtain well-posedness changes - for linearized kinetic half-space problems related to the half-space problem of evaporation and condensation in kinetic theory are considered. The regime transitions correspond to the transition between subsonic and supersonic evaporation/condensation, or the transition between evaporation and condensation. Near the regime transitions, slowly varying modes might occur, preventing uniform exponential speed of convergence there. By imposing extra conditions on the indata at the interface, the slowly varying modes can be eliminated near a regime transition, giving rise to uniform exponential speed of convergence near the regime transition. Values of the velocity of the flow at the far end, for which regime transitions take place are presented for some particular variants of the Boltzmann equation: for monatomic and polyatomic single species and mixtures, and the quantum variant for bosons and fermions.