Uniform shear flow via the Boltzmann equation with hard potentials

The motion of rarefied gases for uniform shear flow at the kinetic level is governed by the spatially homogeneous Boltzmann equation with a deformation force. In this paper, we study the corresponding Cauchy problem with initial data of finite mass and energy for the collision kernel in case of hard potentials $ 0<\gamma\leq 1 $ under the cutoff assumption. We prove the global existence and large time behavior of solutions provided that the force strength $ \alpha>0 $ is small enough. In particular, when the initial perturbation is of order $ \alpha^m $ for $ m>2 $, we make a rigorous justification of the uniform-in-time asymptotic expansion of solutions up to order $ \alpha^2 $ under a homoenergetic self-similar scaling that can capture the increase of temperature $ \theta(t)\sim (1+ \gamma \varrho_0 \alpha^2 t)^{2/\gamma} $ when time tends to infinity, where $ \varrho_0>0 $ is a strictly positive constant depending only on the deformation force and the linearized collision operator. Specifically, we establish$ \begin{aligned} &\theta^{3/2}(t)F(t,\theta^{1/2}(t)v)\\& = \mu+\alpha \sqrt{\mu} G_1(t,v)+\alpha^2 \sqrt{\mu}G_2(t,v)+O(1)\alpha^m(1+ \gamma \varrho_0 \alpha^2 t)^{-2} \end{aligned} $as $ t\to\infty $, where $ \mu $ is a global Maxwellian and $ G_1,G_2 $ are microscopic bounded functions that can be explicitly determined and decay in time as $ G_1\sim (1+ \gamma \varrho_0 \alpha^2 t)^{-1} $ and $ G_2\sim (1+ \gamma \varrho_0 \alpha^2 t)^{-2} $.