Results
HOMAR.Results History
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This work extends
(MHM for short)
in
the decomposition of
of
through an one-field formulation on top
The multiscale
are driven by local Maxwell
magnetic field prescribed on the faces.
Galerkin method in space
Leap-Frog scheme in
the MHM method effective and yields a staggered algorithm within a
divide and conquer framework
to:
We have extended the Multiscale Hybrid-Mixed finite element method
(MHM for short) for dealing with the system of time-domain Maxwell
equations modeling electromagnetic wave propagation in heterogeneous
media. The MHM method arises from the decomposition of the exact
electric and magnetic fields in terms of the solutions of locally
independent Maxwell problems tied together through an one-field
formulation on top of a coarse mesh skeleton. The multiscale basis
functions, which are responsible for upscaling, are driven by local
Maxwell problems with tangential component of the magnetic field
prescribed on the faces. A high order Discontinuous Galerkin method
in space combined with a second order explicit Leap-Frog scheme in
time discretizes the local problems. This makes the MHM method
effective and yields a staggered algorithm within a divide and conquer
framework. The MHM has been formulated for the system of time-domain
Maxwell equations in the three-dimensional case. Preliminary numerical
results have been obtained in the two-dimensional case.
(MHM for short) for dealing with the system of time-domain Maxwell
equations modeling electromagnetic wave propagation in heterogeneous
media. The MHM method arises from the decomposition of the exact
electric and magnetic fields in terms of the solutions of locally
independent Maxwell problems tied together through an one-field
formulation on top of a coarse mesh skeleton. The multiscale basis
functions, which are responsible for upscaling, are driven by local
Maxwell problems with tangential component of the magnetic field
prescribed on the faces. A high order Discontinuous Galerkin method
in space combined with a second order explicit Leap-Frog scheme in
time discretizes the local problems. This makes the MHM method
effective and yields a staggered algorithm within a divide and conquer
framework. The MHM has been formulated for the system of time-domain
Maxwell equations in the three-dimensional case. Preliminary numerical
results have been obtained in the two-dimensional case.
Changed lines 40-43 from:
A MHM formulation has also been proposed and studied for the
system of
to:
A MHM formulation has also been proposed and studied for the system of
time-domain elastodynamic equations in mixed (velocity-stress) form.
Preliminary numerical results have been obtained in the
two-dimensional case.
time-domain elastodynamic equations in mixed (velocity-stress) form.
Preliminary numerical results have been obtained in the
two-dimensional case.
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!!! MHM for the system of time-domain elastodynamic equations\\\
A MHM formulation has also been proposed and studied for the
system of time-domain elastodynamic equations in mixed (velocity-stress) form.
Preliminary numerical results have been obtained in the two-dimensional case.
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For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]]
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For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at WONAPDE 2016]]
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For more details: %newwin% [http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]
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For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]]
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%center% Nanowaveguide problem: coarse quandrangular meshes
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%center% DGTD method with 589,824 DoF (left) and 4,608 DoF (right)
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%center% MHM-DGTD method with 9,216 DoF
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MHM for teh system of time-domain Maxwell equations
to:
!!! MHM for the system of time-domain Maxwell equations\\\
This work extends the Multiscale Hybrid-Mixed finite element method
(MHM for short) for the two- and three-dimensional Maxwell equations
in time-domain with heterogeneous media. The MHM method arises from
the decomposition of the exact electric and magnetic fields in terms
of the solutions of locally independent Maxwell problems tied together
through an one-field formulation on top of a coarse mesh skeleton.
The multiscale basis functions, which are responsible for upscaling,
are driven by local Maxwell problems with tangential component of the
magnetic field prescribed on the faces. A high order Discontinuous
Galerkin method in space combined with a second order explicit
Leap-Frog scheme in time discretizes the local problems. This makes
the MHM method effective and yields a staggered algorithm within a
divide and conquer framework.
Added line 2:
MHM for teh system of time-domain Maxwell equations
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(:title Results:)
to:
(:title Results:)
(:linebreaks:)
[[Main/HOMAR | HOMAR home]]
(:linebreaks:)
[[Main/HOMAR | HOMAR home]]