107 research outputs found
Highly rotating viscous compressible fluids in presence of capillarity effects
In this paper we study a singular limit problem for a Navier-Stokes-Korteweg
system with Coriolis force, in the domain and for general
ill-prepared initial data. Taking the Mach and the Rossby numbers to be
proportional to a small parameter \veps going to , we perform the
incompressible and high rotation limits simultaneously. Moreover, we consider
both the constant capillarity and vanishing capillarity regimes. In this last
case, the limit problem is identified as a -D incompressible Navier-Stokes
equation in the variables orthogonal to the rotation axis. If the capillarity
is constant, instead, the limit equation slightly changes, keeping however a
similar structure. Various rates at which the capillarity coefficient can
vanish are also considered: in most cases this will produce an anisotropic
scaling in the system, for which a different analysis is needed. The proof of
the results is based on suitable applications of the RAGE theorem.Comment: Version 2 includes a corrigendum, which fixes errors contained in the
proofs to Theorems 6.5 and 6.
Existence of global strong solutions for the shallow-water equations with large initial data
This work is devoted to the study of a viscous shallow-water system with
friction and capillarity term. We prove in this paper the existence of global
strong solutions for this system with some choice of large initial data when
in critical spaces for the scaling of the equations. More precisely,
we introduce as in \cite{Hprepa} a new unknown,\textit{a effective velocity}
v=u+\mu\n\ln h ( is the classical velocity and the depth variation of
the fluid) with the viscosity coefficient which simplifies the system and
allow us to cancel out the coupling between the velocity and the depth
variation . We obtain then the existence of global strong solution if
is small in and large in
. In particular it implies that the classical momentum
can be large in , but small when we
project on the divergence field. These solutions are in some sense
\textit{purely compressible}. We would like to point out that the friction term
term has a fundamental role in our work inasmuch as coupling with the pressure
term it creates a damping effect on the effective velocity
Global Existence and Vanishing Dispersion Limit of Strong/Classical Solutions to the One-dimensional Compressible Quantum Navier-Stokes Equations with Large Initial Data
We are concerned with the global existence and vanishing dispersion limit of
strong/classical solutions to the Cauchy problem of the one-dimensional
barotropic compressible quantum Navier-Stokes equations, which consists of the
compressible Navier-Stokes equations with a linearly density-dependent
viscosity and a nonlinear third-order differential operator known as the
quantum Bohm potential. The pressure is considered with
being a constant. We focus on the case when the viscosity
constant and the Planck constant are not equal. Under some
suitable assumptions on , and the initial data, we
proved the global existence and large-time behavior of strong and classical
solutions away from vacuum to the compressible quantum Navier-Stokes equations
with arbitrarily large initial data. This result extends the previous ones on
the construction of global strong large-amplitude solutions of the compressible
quantum Navier-Stokes equations to the case . Moreover, the
vanishing dispersion limit for the classical solutions of the quantum
Navier-Stokes equations is also established with certain convergence rates. The
proof is based on a new effective velocity which converts the quantum
Navier-Stokes equations into a parabolic system, and some elaborate estimates
to derive the uniform-in-time positive lower and upper bounds on the specific
volume.Comment: 40page
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