Well-posedness and stability of the Navier-Stokes-Maxwell equations
arxiv(2024)
摘要
The paper is devoted to studying the well-posedness and stability of the
generalized Navier-Stokes-Maxwell (NSM) equations with the standard Ohm's law
in ℝ^d for d ∈{2,3}. More precisely, the global
well-posedness is established in case of fractional Laplacian velocity
(-Δ)^α v with α = d/2 for suitable data. In
addition, the local well-posedness in the inviscid case is also provided for
sufficient smooth data, which allows us to study the inviscid limit of
associated positive viscosity solutions in the case α = 1, where an
explicit bound on the difference is given. On the other hand, in the case
α = 0 the stability near a magnetohydrostatic equilibrium with a
constant (or equivalently bounded) magnetic field is also obtained in which
nonhomogeneous Sobolev norms of the velocity and electric fields, and the
L^∞ norm of the magnetic field converge to zero as time goes to infinity
with an implicit rate. In this velocity damping case, the situation is
different both in case of the two and a half, and three-dimensional
magnetohydrodynamics (MHD) system, where an explicit rate of convergence in
infinite time is computed for both the velocity and magnetic fields in
nonhomogeneous Sobolev norms. Therefore, there is a gap between NSM and MHD in
terms of the norm convergence of the magnetic field and the rate of decaying in
time, even the latter equations can be proved as a limiting system of the
former one in the sense of distributions as the speed of light tends to
infinity.
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