We consider the displacement of an electronic cloud generated by the local
difference of charge with a uniform neutralizing background of non-moving i
ons. The equations are given by the Vlasov-Poisson system, with a coupling
constant epsilon = (tau/2 pi)(2) where tau is the (constant) oscillation pe
riod of the electrons. In the so-called quasi-neutral regime, namely as eps
ilon --> 0, the current is expected to converge to a solution of the incomp
ressible Euler equations, at least in the case of a vanishing initial tempe
rature. This result is proved by adapting an argument used by P.-L. Lions [
Li] to prove the convergence of the Leray solutions of the 3d Navier-Stokes
equation to the so-called dissipative solutions of the Euler equations. Fo
r this purpose, the total energy of the system is modulated by a test-funct
ion. An alternative proof is given, based on the concept of measure-valued
(mv) solutions introduced by DiPerna and Majda [DM] and already used by Bre
nier and Grenier [BG], [Gr2] for the asymptotic analysis of the Vlasov-Pois
son system in the quasi-neutral regime. Through this analysis, a link is es
tablished between Lions' dissipative solutions and Diperna-Majda's my solut
ions of the Euler equations. A second interesting asymptotic regime, still
leading to the Euler equations, known as the gyrokinetic limit of the Vlaso
v-Poisson system, is obtained when the electrons are forced by a strong con
stant external magnetic field and has been investigated in [Gr3], [GSR]. As
for the quasi-neutral limit, we justify the gyrokinetic limit by using the
concepts of dissipative solutions and modulated total energy.