Abstract

In this paper, we are concerned with the initial boundary valueproblem on the two-fluid Navier-Stokes-Poisson system in thehalf-line $R_+$. We establish the global-in-time asymptoticstability of the rarefaction wave and the boundary layer both forthe outflow problem under the smallness assumption on initialperturbation, where the strength of the rarefaction wave is notnecessarily small while the strength of the boundary layer isadditionally supposed to be small. Here, the large initial data withdensities far from vacuum is also allowed in the case of thenon-degenerate boundary layer. The results show that the large-timebehavior of solutions coincides with the one for the singleNavier-Stokes system in the absence of the electric field. The proofis based on the classical energy method. The main difficulty in theanalysis comes from the slower time-decay rate of the system causedby the appearance of the electric field. To overcome it, we use thecoupling property of the two-fluid equations to capture thedissipation of the electric field interacting with the nontrivialasymptotic profile.

Highlights

  • The two-fluid Navier-Stokes-Poisson system is a model used to simulate the transport of charged particles

  • Our goal in this paper is to study the large time behavior of global solutions to the IBVP on the two-fluid NSP system (1)

  • Compared with the case of the single quasineutral Navier-Stokes system (2), we mainly investigate the influence of the electric field on the time asymptotic stability of some nontrivial profiles

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Summary

Introduction

The two-fluid Navier-Stokes-Poisson (called NSP in the sequel for simplicity) system is a model used to simulate the transport of charged particles (e.g., electrons and ions). One way for estimating (9) is to make use of the time-space integrability of the first-order space derivative of E in terms of the possible space-decay property of u∞(x, t) at infinity together with the Hardy inequality It is the case in the study of the stability of the non-degenerate boundary layer, see the proof of Theorem 3.4. It should be pointed out that system (1) in the non-dimensional form depends generally on the ratios of masses, charges and temperatures of two fluids and on the Debye length, cf [26] and [1] In such case, the two-fluid plasma system exhibits more complex coupling structure and the corresponding analysis of the large time behavior of solutions becomes more complicated [3].

Riemann problem on the
The above estimates imply t
The last term in the above equation can be rewritten as
It is straightforward to see
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