Abstract:We study the Hilbert expansion for small Knudsen number $\varepsilon$ for the
Vlasov-Boltzmann-Poisson system for an electron gas. The zeroth order term
takes the form of local Maxwellian: $ F_{0}(t,x,v)=\frac{\rho_{0}(t,x)}{(2\pi
\theta_{0}(t,x))^{3/2}} e^{-|v-u_{0}(t,x)|^{2}/2\theta_{0}(t,x)},\text{\
}\theta_{0}(t,x)=K\rho_{0}^{2/3}(t,x).$ Our main result states that if the
Hilbert expansion is valid at $t=0$ for well-prepared small initial data with
irrotational velocity $u_0$, then it is valid for $0\leq t… Show more
“…For any large m ≫ 1 we define k ̺,m (v, u) = 1 |v−u|≥ 1 m ,|v|≤m k ̺ (v, u), (8.17) such that sup v´R3 |k ̺,m (v, u) − k ̺ (v, u)|du 1 m , and |k ̺,m (v, u)| m 1. Furthermore we split the time interval as, for each ℓ, l 18)…”
Section: From (83)mentioning
confidence: 99%
“…18), (4.23), and (4.24), the contribution of |Γ(∂f, f )| + |Γ gain (f, ∂f )| + |K∂f | of (4.43) in (4.44) G is bounded by…”
When dilute charged particles are confined in a bounded domain, boundary effects are crucial in the global dynamics. We construct a unique global-in-time solution to the Vlasov-Poisson-Boltzmann system in convex domains with the diffuse boundary condition. The construction is based on an L 2 -L ∞ framework with a novel nonlinear-normed energy estimate of a distribution function in weighted W 1,p -spaces and a C 2,δ -estimate of the self-consistent electric potential. Moreover we prove an exponential convergence of the distribution function toward the global Maxwellian.
“…For any large m ≫ 1 we define k ̺,m (v, u) = 1 |v−u|≥ 1 m ,|v|≤m k ̺ (v, u), (8.17) such that sup v´R3 |k ̺,m (v, u) − k ̺ (v, u)|du 1 m , and |k ̺,m (v, u)| m 1. Furthermore we split the time interval as, for each ℓ, l 18)…”
Section: From (83)mentioning
confidence: 99%
“…18), (4.23), and (4.24), the contribution of |Γ(∂f, f )| + |Γ gain (f, ∂f )| + |K∂f | of (4.43) in (4.44) G is bounded by…”
When dilute charged particles are confined in a bounded domain, boundary effects are crucial in the global dynamics. We construct a unique global-in-time solution to the Vlasov-Poisson-Boltzmann system in convex domains with the diffuse boundary condition. The construction is based on an L 2 -L ∞ framework with a novel nonlinear-normed energy estimate of a distribution function in weighted W 1,p -spaces and a C 2,δ -estimate of the self-consistent electric potential. Moreover we prove an exponential convergence of the distribution function toward the global Maxwellian.
“…Recently, a new model called the INSF system with viscous heating was derived by Bardos-Levermore-Ukai-Yang [4]. The aim of the present paper is to justify such an incompressible hydrodynamic approximation to the Boltzmann equation in a periodic box via an L 2 − L ∞ method developed in [12,13,21,22,23,24]. We now outline a few key points of the paper which are distinct to some extent with the previous work by Bardos-Levermore-Ukai-Yang [4]:…”
The incompressible Navier-Stokes-Fourier system with viscous heating was first derived from the Boltzmann equation in the form of the diffusive scaling by Bardos-Levermore- . The purpose of this paper is to justify such an incompressible hydrodynamic approximation to the Boltzmann equation in L 2 ∩ L ∞ setting in a periodic box. Based on an odd-even expansion of the solution with respect to the microscopic velocity, the diffusive coefficients are determined by the incompressible Navier-Stokes-Fourier system with viscous heating and the super Burnett functions. More importantly, the remainder of the expansion is proven to decay exponentially in time via an L 2 − L ∞ approach on the condition that the initial data satisfies the mass, momentum and energy conversation laws.2010 Mathematics Subject Classification. 35Q20, 35Q79, 35C20.
“…On the other hand, the NSP system at the fluid level can be justified by taking the hydrodynamical limit of the Vlasov-type Boltzmann equation by the Chapman-Enskog expansion, cf. [4,17,18,19]. In recent years, there have been a great number of mathematical studies of the NSP system.…”
This paper is concerned with the study of the nonlinear stability of the contact discontinuity of the Navier-Stokes-Poisson system with free boundary in the case where the electron background density satisfies an analogue of the Boltzmann relation. We especially allow that the electric potential can take distinct constant states at boundary. On account of the quasineutral assumption, we first construct a viscous contact wave through the quasineutral Euler equations, and then prove that such a non-trivial profile is time-asymptotically stable under small perturbations for the corresponding initial boundary value problem of the Navier-Stokes-Poisson system. The analysis is based on the techniques developed in [11] and an elementary L 2 energy method.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.