PmWiki
HOMAR

Results

HOMAR.Results History

Hide minor edits - Show changes to output

October 18, 2017, at 08:57 AM by 138.96.200.15 -
Changed lines 49-51 from:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t2.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t3.png
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t4.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t5.png
to:
%center% %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
%center% %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t2.png %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t3.png
%center% %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t4.png %width=320px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t5.png
October 18, 2017, at 08:36 AM by 138.96.200.15 -
Added line 4:
Added line 41:
October 18, 2017, at 08:36 AM by 138.96.200.15 -
Changed lines 4-18 from:

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
.
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
.
Changed lines 40-43 from:

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.
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.
October 18, 2017, at 08:32 AM by 138.96.200.15 -
Deleted lines 41-45:

>>frame bgcolor='white'<<

%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-coarse.png %width=280px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-fine.png
>><<
October 18, 2017, at 08:32 AM by 138.96.200.15 -
Changed lines 45-49 from:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-coarse.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-fine.png
to:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-coarse.png %width=280px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-fine.png
>><<

>>frame bgcolor='white'<<

October 18, 2017, at 08:31 AM by 138.96.200.15 -
Added line 45:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-coarse.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/complex-fine.png
October 18, 2017, at 08:30 AM by 138.96.200.15 -
Changed line 23 from:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png
to:
%center% %width=230px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png %width=230px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png
Changed line 29 from:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/dg_6.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/dg_9.png
to:
%center% %width=230px% http://www-sop.inria.fr/nachos/pics/homar/dg_6.png %width=230px% http://www-sop.inria.fr/nachos/pics/homar/dg_9.png
Changed line 31 from:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png
to:
%center% %width=230px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png
October 18, 2017, at 08:29 AM by 138.96.200.15 -
Changed lines 46-47 from:
%width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t2.png
to:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t2.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t3.png
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t4.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t5
.png
October 18, 2017, at 08:28 AM by 138.96.200.15 -
Changed lines 45-46 from:
%center% %width=250px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=250px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
to:
%center% %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
%width=300px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t2.png
October 18, 2017, at 08:28 AM by 138.96.200.15 -
Changed line 45 from:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
to:
%center% %width=250px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=250px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
October 18, 2017, at 08:27 AM by 138.96.200.15 -
October 18, 2017, at 08:27 AM by 138.96.200.15 -
Added lines 36-46:

!!! 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.

>>frame bgcolor='white'<<

%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t0.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/elasto/t1.png
>><<
October 17, 2017, at 04:47 PM by 138.96.200.15 -
Changed line 19 from:
For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]]
to:
For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at WONAPDE 2016]]
October 17, 2017, at 04:46 PM by 138.96.200.15 -
Changed line 19 from:
For more details: %newwin% [http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]
to:
For more details: %newwin% [[http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]]
October 17, 2017, at 04:45 PM by 138.96.200.15 -
Added lines 18-19:

For more details: %newwin% [http://www-sop.inria.fr/nachos/slides/Wonapde_2016-DParedes.pdf | slides of Diego Paredes presentation at Wonapde 2016]
October 17, 2017, at 04:32 PM by 138.96.200.15 -
Added line 26:
October 17, 2017, at 04:32 PM by 138.96.200.15 -
Added line 20:
October 17, 2017, at 04:31 PM by 138.96.200.15 -
Deleted line 25:
Deleted line 26:
Deleted line 27:
October 17, 2017, at 04:31 PM by 138.96.200.15 -
Deleted line 20:
October 17, 2017, at 04:31 PM by 138.96.200.15 -
Added lines 21-22:

%center% Nanowaveguide problem: coarse quandrangular meshes
Added line 24:
Added lines 28-29:
%center% DGTD method with 589,824 DoF (left) and 4,608 DoF (right)
Added lines 31-32:

%center% MHM-DGTD method with 9,216 DoF
October 17, 2017, at 04:22 PM by 138.96.200.15 -
Changed line 20 from:
%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png %width=260px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png
to:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png
Changed lines 23-25 from:
%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/dg_6.png %width=260px% http://www-sop.inria.fr/nachos/pics/homar/dg_9.png

%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png
to:
%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/dg_6.png %width=200px% http://www-sop.inria.fr/nachos/pics/homar/dg_9.png

%center% %width=200px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png
October 17, 2017, at 04:18 PM by 138.96.200.15 -
Added lines 24-25:

%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png
October 17, 2017, at 04:17 PM by 138.96.200.15 -
Added lines 21-23:
>><<
>>frame bgcolor='white'<<
%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/dg_6.png %width=260px% http://www-sop.inria.fr/nachos/pics/homar/dg_9.png
October 17, 2017, at 04:17 PM by 138.96.200.15 -
Added lines 18-21:

>>frame bgcolor='white'<<
%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png %width=260px% http://www-sop.inria.fr/nachos/pics/homar/ten_quad4edge_balls-eps-converted-to.png
>><<
October 17, 2017, at 04:16 PM by 138.96.200.15 -
Changed lines 2-17 from:
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.
October 17, 2017, at 04:15 PM by 138.96.200.15 -
Added line 2:
MHM for teh system of time-domain Maxwell equations
July 18, 2015, at 09:20 AM by 82.228.254.112 -
Changed lines 1-5 from:
(:title Results:)
to:
(:title Results:)

(:linebreaks:)

[[Main/HOMAR | HOMAR home]]
July 16, 2015, at 09:08 AM by 82.228.254.112 -
Added line 1:
(:title Results:)