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The Navier–Stokes equations are approximated by means of
a fractional step, Chorin–Temam projection method; the time derivative
is approximated by a three-level backward finite difference, whereas
the approximation in space is performed by a Galerkin technique.
It is shown that the proposed scheme yields an error
of
for the velocity in the norm of
(L(Ω)), where ≥ 1 is
the polynomial degree of the velocity approximation. It is also shown
that the splitting error of projection...
This paper presents a
stabilization technique for approximating transport
equations. The key idea consists in introducing an artificial diffusion
based on a two-level decomposition of the approximation space.
The technique is proved to have stability and convergence
properties that are similar to that of the streamline diffusion method.
We show that the Maxwell equations in the low frequency limit, in a domain composed of insulating and conducting regions, has a saddle point structure, where the electric field in the insulating region is the Lagrange multiplier that enforces the curl-free constraint on the magnetic field. We propose a mixed finite element technique for solving this problem, and we show that, under mild regularity assumption on the data, Lagrange finite elements can be used as an alternative to edge elements.
This paper presents a model based on spectral hyperviscosity for the simulation of 3D turbulent incompressible flows. One particularity of this model is that the hyperviscosity is active only at the short velocity scales, a feature which is reminiscent of Large Eddy Simulation models. We propose a Fourier–Galerkin approximation of the perturbed Navier–Stokes equations and we show that, as the cutoff wavenumber goes to infinity, the solution of the model converges (up to subsequences) to a weak solution...
This paper presents a model based on spectral hyperviscosity for the
simulation of 3D turbulent incompressible flows. One particularity of this
model is that the hyperviscosity is active only at the short velocity scales,
a feature which is reminiscent of Large Eddy Simulation models.
We propose a Fourier–Galerkin approximation of the perturbed
Navier–Stokes equations and we show that, as the cutoff wavenumber
goes to infinity, the solution of the model
converges (up to subsequences) to a weak...
We show that the Maxwell equations
in the low frequency limit, in a domain composed of insulating
and conducting regions, has a saddle point structure, where
the electric field in the insulating region is the Lagrange
multiplier that enforces the curl-free constraint on the magnetic field.
We propose a mixed finite element technique
for solving this problem, and we show that, under mild regularity
assumption on the data, Lagrange finite elements can be used
as an alternative to edge elements.
This paper derives upper and lower bounds for the -condition
number of the stiffness matrix resulting from the finite element
approximation of a linear, abstract model problem. Sharp estimates in
terms of the meshsize are obtained. The theoretical results are
applied to finite element approximations of elliptic PDE's in
variational and in mixed form, and to first-order PDE's approximated
using the Galerkin–Least Squares technique or by
means of a non-standard Galerkin technique in
...
This work is devoted to the study of a two-dimensional vector
Poisson equation with the normal component of the unknown and
the value of the divergence of the unknown prescribed simultaneously
on the entire boundary.
These two scalar boundary conditions appear
alternative in a standard variational framework. An original
variational formulation of this boundary value problem
is proposed here. Furthermore, an uncoupled solution algorithm is
introduced together with its finite element approximation.
The...
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