PmWiki | HORSE | History

November 25, 2016, at 08:21 AM by 138.96.200.15 -

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%center% Scattering of a plane wave by the Lockheed F-104 Starfighter, Frequency of the incident wave: 600 MHz. Unstructured tetrahedral mesh with 1,645,874 elements and 3,521,251 faces.

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%center% Scattering of a plane wave by the Lockheed F-104 Starfighter. Frequency of the incident wave: 600 MHz. Unstructured tetrahedral mesh with 1,645,874 elements and 3,521,251 faces.

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(:linebreaks:)

%center% Scattering of a plane wave by the Lockheed F-104 Starfighter. Frequency of the incident wave: 600 MHz. Strong scalability analysis: Occigen Bull/Atos cluster at CINES, Intel E5-2690, 2.6~GHz, 24 cores on each node, 64 GB or 128 GB RAM per node.

November 25, 2016, at 08:15 AM by 138.96.200.15 -

November 25, 2016, at 08:14 AM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~250px~~% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png

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(:cellnr align='center':) %width=275px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png

November 25, 2016, at 08:13 AM by 138.96.200.15 -

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(:cell align='center':) %width=~~300px~~% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

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(:cell align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

November 25, 2016, at 08:13 AM by 138.96.200.15 -

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(:cell align='center':) %width=~~275px~~% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

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(:cell align='center':) %width=300px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

November 25, 2016, at 08:13 AM by 138.96.200.15 -

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(:cellnr align='center':) Characteristics of uniform tetrahdral meshes

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(:cellnr align='center':) Characteristics of uniform tetrahdral meshes used for the numerical convergence study.

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(:cellnr align='center':) used for the numerical convergence study.
(:cell align='center':)

November 25, 2016, at 08:12 AM by 138.96.200.15 -

Changed line 15 from:

(:cellnr align='center':) Characteristics of uniform tetrahdral meshes ~~usded for the numerical convergence study.~~

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(:cellnr align='center':) Characteristics of uniform tetrahdral meshes

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(:cellnr align='center':) used for the numerical convergence study.
(:cell align='center':)

November 25, 2016, at 08:12 AM by 138.96.200.15 -

Changed line 14 from:

(:cell align='center':) %width=~~250px~~% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

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(:cell align='center':) %width=275px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

November 25, 2016, at 08:11 AM by 138.96.200.15 -

Added line 14:

(:cell align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

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(:cell align='center':) Size of the discrete HDG systems for mesh M4.

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(:linebreaks:)

(:table align='center' border='5px' bordercolor='black' width='100%' bgcolor='ivory':)
(:cellnr align='center':) \# DoF
(:cell align='center':) HDG-P1
(:cell align='center':) HDG-P2
(:cell align='center':) HDG-P3
(:cellnr align='center':) Hybrid variable
(:cell align='center':) 21,127,506
(:cell align='center':) 42,255,012
(:cell align='center':) 70,425,020
(:cellnr align='center':) ('''E''''_h_' , '''H''''_h_')
(:cell align='center':) 39,500,976
(:cell align='center':) 98,752,440
(:cell align='center':) 197,504,880
(:tableend:)

November 25, 2016, at 08:02 AM by 138.96.200.15 -

Deleted lines 14-16:

(:cellnr align='center':)
(:cellnr align='center':) %width=500px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg
(:cellnr align='center':) HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

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(:linebreaks:)

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(:cellnr align='center':) %width=500px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg
(:cellnr align='center':) HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.
(:tableend:)

(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)

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(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=300px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png
(:cellnr align='center':)
(:tableend:)

November 25, 2016, at 08:00 AM by 138.96.200.15 -

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(:cellnr align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png
(:cellnr align='center':)

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(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=300px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png
(:cellnr align='center':)
(:tableend:)

November 25, 2016, at 07:58 AM by 138.96.200.15 -

Changed lines 31-32 from:

(:~~cell~~ align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.~~png~~

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(:cellnr align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png
(:cellnr align='center':)

November 25, 2016, at 07:58 AM by 138.96.200.15 -

Added line 31:

(:cell align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_DoF.png

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%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver, GMRES accelerated %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

to:

%center% HDG method for the three-dimensional frequency-domain Maxwell equations. Plane wave propagation in vacuum. Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver, GMRES accelerated %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

Deleted lines 36-54:

(:table align='center' border='5px' bordercolor='black' width='100%' bgcolor='ivory':)
(:cellnr align='center':) \# DoF
(:cell align='center':) HDG-P1
(:cell align='center':) HDG-P2
(:cell align='center':) HDG-P3
(:cell align='center':) HDG-P4
(:cellnr align='center':) Hybrid variable
(:cell align='center':) 257,472
(:cell align='center':) 514,944
(:cell align='center':) 858,240
(:cell align='center':) 1,287,360
(:cellnr align='center':) ('''E''''_h_' , '''H''''_h_')
(:cell align='center':) 497,664
(:cell align='center':) 1,244,160
(:cell align='center':) 2,488,320
(:cell align='center':) 4,354,560
(:tableend:)

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~~(:linebreaks:)~~

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%center% Scattering of a plane wave by the Lockheed F-104 ~~Starfight~~, Frequency of the incident wave: 600 MHz. Unstructured tetrahedral mesh with 1,645,874 elements and 3,521,251 faces.

to:

%center% Scattering of a plane wave by the Lockheed F-104 Starfighter, Frequency of the incident wave: 600 MHz. Unstructured tetrahedral mesh with 1,645,874 elements and 3,521,251 faces.

November 25, 2016, at 07:54 AM by 138.96.200.15 -

Changed lines 12-17 from:

~~%lfloat text-align~~=~~center~~ width=~~250px~~% ~~http~~://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

(:linebreaks:)
(:linebreaks:)

%lfloat text-~~align=center width=500px% http://www-~~sop.inria.fr/nachos/softs/horse/pw_~~conv~~.~~jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical~~ convergence ~~analysis considering the simple problem of a plane wave propagation in vacuum~~. ~~A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.~~

to:

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png
(:cellnr align='center':) Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.
(:cellnr align='center':)
(:cellnr align='center':) %width=500px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg
(:cellnr align='center':) HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.
(:tableend:)

November 25, 2016, at 07:52 AM by 138.96.200.15 -

Changed line 12 from:

%lfloat width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

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%lfloat text-align=center width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 25, 2016, at 07:52 AM by 138.96.200.15 -

Changed line 12 from:

%lfloat ~~text-align=right~~ width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

to:

%lfloat width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 25, 2016, at 07:52 AM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=~~left~~ width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

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%lfloat text-align=right width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 25, 2016, at 07:51 AM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=~~center~~ width=~~300px~~% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

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%lfloat text-align=left width=250px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 25, 2016, at 07:51 AM by 138.96.200.15 -

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%lfloat text-align=center width=~~500px~~% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

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%lfloat text-align=center width=300px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

(:linebreaks:)
(:linebreaks:)

November 25, 2016, at 07:50 AM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=500px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.~~jpg~~ | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

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%lfloat text-align=center width=500px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 25, 2016, at 07:50 AM by 138.96.200.15 -

Added lines 11-12:

%lfloat text-align=center width=500px% http://www-sop.inria.fr/nachos/softs/horse/size_mesh.jpg | Characteristics of uniform tetrahdral meshes usded for the numerical convergence study.

November 23, 2016, at 07:54 AM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~450px~~% http://www-sop.inria.fr/nachos/softs/horse/DoF_F-104.png

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(:cellnr align='center':) %width=400px% http://www-sop.inria.fr/nachos/softs/horse/DoF_F-104.png

November 23, 2016, at 07:54 AM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~600px~~% http://www-sop.inria.fr/nachos/softs/horse/DoF_F-104.png

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(:cellnr align='center':) %width=450px% http://www-sop.inria.fr/nachos/softs/horse/DoF_F-104.png

November 23, 2016, at 07:53 AM by 138.96.200.15 -

Added lines 82-85:

(:cellnr align='center':) %width=600px% http://www-sop.inria.fr/nachos/softs/horse/DoF_F-104.png
(:cellnr align='center':) Size of the discrete HDG systems
(:cellnr align='center':)
(:cellnr align='center':)

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(:cellnr align='center':)

November 22, 2016, at 05:18 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~650px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

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(:cellnr align='center':) %width=600px% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

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(:cellnr align='center':) %width=~~575px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png

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(:cellnr align='center':) %width=500px% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png

November 22, 2016, at 05:18 PM by 138.96.200.15 -

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(:cellnr align='center':)

November 22, 2016, at 05:17 PM by 138.96.200.15 -

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(:linebreaks:)

November 22, 2016, at 05:15 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~600px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png

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(:cellnr align='center':) %width=575px% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png

November 22, 2016, at 05:14 PM by 138.96.200.15 -

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%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver, GMRES accelerated %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with ~~MUMPS~~ as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

to:

%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver, GMRES accelerated %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

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(:cellnr align='center':) %width=~~650px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png
(:cellnr align='center':) %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with ~~MUMPS~~ as a local sparse direct solver

to:

(:cellnr align='center':) %width=600px% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png
(:cellnr align='center':) %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with PaStiX as a local sparse direct solver

November 22, 2016, at 05:13 PM by 138.96.200.15 -

Changed lines 82-83 from:

(:cellnr align='center':) [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with ~~PaStiX as a local sparse direct~~ solver

to:

(:cellnr align='center':) %newwin% [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver
(:cellnr align='center':) %width=650px% http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png
(:cellnr align='center':) %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with MUMPS as a local sparse direct solver

November 22, 2016, at 05:11 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~425px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

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(:cellnr align='center':) %width=650px% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

November 22, 2016, at 05:11 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~325px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

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(:cellnr align='center':) %width=425px% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png

November 22, 2016, at 05:11 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~375px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=~~375px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

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(:cellnr align='center':) %width=355px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=355px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

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(:cellnr align='center':) %width=~~375px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png
(:cell align='center':) %width=~~375px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P4.png

to:

(:cellnr align='center':) %width=355px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png
(:cell align='center':) %width=355px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P4.png

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(:tableend:)

to:

(:tableend:)

(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=325px% http://www-sop.inria.fr/nachos/softs/horse/F-104_MaPHyS+PaStiX.png
(:cellnr align='center':) [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with PaStiX as a local sparse direct solver

(:tableend:)

November 22, 2016, at 05:05 PM by 138.96.200.15 -

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(:cellnr align='center':) HDG-P2 method
(:cell align='center':) HDG-P3 method

November 22, 2016, at 04:59 PM by 138.96.200.15 -

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(:tableend:)

%center% Scattering of a plane wave by the Lockheed F-104 Starfight, Frequency of the incident wave: 600 MHz. Unstructured tetrahedral mesh with 1,645,874 elements and 3,521,251 faces.

(:linebreaks:)

(:table align='center' border='5px' bordercolor='black' width='100%' bgcolor='ivory':)
(:cellnr align='center':) \# DoF
(:cell align='center':) HDG-P1
(:cell align='center':) HDG-P2
(:cell align='center':) HDG-P3
(:cellnr align='center':) Hybrid variable
(:cell align='center':) 21,127,506
(:cell align='center':) 42,255,012
(:cell align='center':) 70,425,020
(:cellnr align='center':) ('''E''''_h_' , '''H''''_h_')
(:cell align='center':) 39,500,976
(:cell align='center':) 98,752,440
(:cell align='center':) 197,504,880

November 22, 2016, at 04:53 PM by 138.96.200.15 -

Changed lines 53-54 from:

(:cellnr align='center':) %width=~~375px~~% http://www-sop.inria.fr/nachos/softs/horse/F-104View1-P2ScaleP3.png

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(:cellnr align='center':) %width=325px% http://www-sop.inria.fr/nachos/softs/horse/F-104View1-P2ScaleP3.png
(:cell align='center':) %width=325px% http://www-sop.inria.fr/nachos/softs/horse/F-104View1-P3.png

November 22, 2016, at 04:02 PM by 138.96.200.15 -

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(:tableend:)

(:linebreaks:)
(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=375px% http://www-sop.inria.fr/nachos/softs/horse/F-104View1-P2ScaleP3.png

November 22, 2016, at 03:56 PM by 138.96.200.15 -

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%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local (sparse direct) solver,

to:

%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local sparse direct solver, GMRES accelerated %newwin% [[http://dx.doi.org/10.1016/j.jcp.2013.09.003 | Schwarz]] algorithm with MUMPS as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

November 22, 2016, at 03:52 PM by 138.96.200.15 -

Changed line 27 from:

%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network.

to:

%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network. Solutions strategies for the hybrid variable system (globally coupled unknowns): %newwin% [[http://mumps.enseeiht.fr | MUMPS]] sparse direct solver, [[http://maphys.gforge.inria.fr | MaPHyS]] algebraic hybrid iterative-direct solver with MUMPS or [[http://pastix.gforge.inria.fr/files/README-txt.html | PaStiX]] as a local (sparse direct) solver,

November 22, 2016, at 03:47 PM by 138.96.200.15 -

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%center% Strong scalability analysis

to:

%center% Strong scalability analysis: %newwin% [[https://www.plafrim.fr/en/home | cluster]] with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network.

(:linebreaks:)

Changed line 37 from:

(:cellnr align='center':) ~~'''ƈ'''~~

to:

(:cellnr align='center':) Hybrid variable

November 22, 2016, at 03:36 PM by 138.96.200.15 -

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(:cellnr align='center':) '''&#~~39B~~;'''

to:

(:cellnr align='center':) '''ƈ'''

November 22, 2016, at 03:35 PM by 138.96.200.15 -

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(:table ~~border~~='0' ~~width~~='~~100%~~' ~~align~~='~~center~~' ~~cellspacing~~='~~1px~~':)

to:

(:table align='center' border='5px' bordercolor='black' width='100%' bgcolor='ivory':)

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(:cellnr align='center':) '''&#~~396~~;'''

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(:cellnr align='center':) '''&#39B;'''

November 22, 2016, at 03:33 PM by 138.96.200.15 -

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(:cellnr align='center':) '''&#396'''

to:

(:cellnr align='center':) '''ƌ'''

November 22, 2016, at 03:33 PM by 138.96.200.15 -

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(:cellnr align='center':) '''&#0396'''

to:

(:cellnr align='center':) '''&#396'''

November 22, 2016, at 03:32 PM by 138.96.200.15 -

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%~~left~~% Strong scalability analysis
~~%left% \# DoF (Degrees of Freedom~~) ~~for the hybrid variable~~ (~~globally coupled unknowns): 257,472 (~~HDG-P1~~); 514,944 (HDG-P2); 858,240 (~~HDG-P3); 1,287,360 (HDG-P4)
%left% \# DoF for (''~~'E''''_h_' ,~~ '''H''''~~_h_~~'): ~~497,664 (HDG-P1); 1~~,~~244,160~~ (~~HDG-P2); 2,488,320 (HDG-P3); 4~~,~~354,560~~ (~~HDG-P4~~)

to:

%center% Strong scalability analysis

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) \# DoF
(:cell align='center':) HDG-P1
(:cell align='center':) HDG-P2
(:cell align='center':) HDG-P3
(:cell align='center':) HDG-P4
(:cellnr align='center':) '''&#0396'''
(:cell align='center':) 257,472
(:cell align='center':) 514,944
(:cell align='center':) 858,240
(:cell align='center':) 1,287,360
(:cellnr align='center':) ('''E''''_h_' , '''H''''_h_')
(:cell align='center':) 497,664
(:cell align='center':) 1,244,160
(:cell align='center':) 2,488,320
(:cell align='center':) 4,354,560
(:tableend:)

November 22, 2016, at 03:25 PM by 138.96.200.15 -

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%~~center~~% Strong scalability analysis. \# DoF (Degrees of Freedom) for the hybrid variable (globally coupled unknowns): 257,472 (HDG-P1); 514,944 (HDG-P2); 858,240 (HDG-P3); 1,287,360 (HDG-P4). \# DoF for ('''E''''_h_' , '''H''''_h_'): 497,664 (HDG-P1); 1,244,160 (HDG-P2); 2,488,320 (HDG-P3); 4,354,560 (HDG-P4).

to:

%left% Strong scalability analysis
%left% \# DoF (Degrees of Freedom) for the hybrid variable (globally coupled unknowns): 257,472 (HDG-P1); 514,944 (HDG-P2); 858,240 (HDG-P3); 1,287,360 (HDG-P4)
%left% \# DoF for ('''E''''_h_' , '''H''''_h_'): 497,664 (HDG-P1); 1,244,160 (HDG-P2); 2,488,320 (HDG-P3); 4,354,560 (HDG-P4)

November 22, 2016, at 03:24 PM by 138.96.200.15 -

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%center% Strong scalability analysis. \# DoF (Degrees of Freedom) for the hybrid variable (globally coupled unknowns): 257,472 (HDG-P1); 514,944 (HDG-P2); 858,240 (HDG-P3); 1,287,360 (HDG-P4). \# DoF for ('''E''''_h_' , '''H''''_h_'): 497,664 (HDG-P1); 1,244,160 (HDG-P2); 2,488,320 (HDG-P3); 4,354,560 (HDG-P4).

November 22, 2016, at 03:18 PM by 138.96.200.15 -

Changed lines 21-22 from:

(:cellnr align='center':) %width=~~350px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png
(:cell align='center':) %width=~~350px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P4.png

to:

(:cellnr align='center':) %width=375px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png
(:cell align='center':) %width=375px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P4.png

November 22, 2016, at 03:17 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~350px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=~~350px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

to:

(:cellnr align='center':) %width=375px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=375px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

November 22, 2016, at 03:16 PM by 138.96.200.15 -

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(:cell align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png

to:

(:cell align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

Added lines 21-24:

(:cellnr align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png
(:cell align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P4.png
(:cellnr align='center':) HDG-P3 method
(:cell align='center':) HDG-P4 method

November 22, 2016, at 03:14 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~300px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=~~300px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cellnr align='center':) ~~DGTD~~ method ~~with affine elements~~

to:

(:cellnr align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=350px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cellnr align='center':) HDG-P1 method
(:cell align='center':) HDG-P2 method

November 22, 2016, at 03:14 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=~~400px~~% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png

to:

(:cellnr align='center':) %width=300px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png
(:cell align='center':) %width=300px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png

November 22, 2016, at 03:13 PM by 138.96.200.15 -

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(:cellnr align='center':) %width=400px% http://www-sop.inria.fr/nachos~~/results~~/softs/horse/PW_TimesBest_P1.png

to:

(:cellnr align='center':) %width=400px% http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png

November 22, 2016, at 03:13 PM by 138.96.200.15 -

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(:linebreaks:)

(:table border='0' width='100%' align='center' cellspacing='1px':)
(:cellnr align='center':) %width=400px% http://www-sop.inria.fr/nachos/results/softs/horse/PW_TimesBest_P1.png
(:cellnr align='center':) DGTD method with affine elements
(:tableend:)

November 22, 2016, at 03:11 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=~~400px~~% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

to:

%lfloat text-align=center width=500px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

November 22, 2016, at 01:50 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=~~350px~~% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

to:

%lfloat text-align=center width=400px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

November 22, 2016, at 01:50 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=~~450px~~% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

to:

%lfloat text-align=center width=350px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

November 22, 2016, at 01:22 PM by 138.96.200.15 -

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%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum. A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

November 22, 2016, at 01:09 PM by 138.96.200.15 -

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%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field, and '''H''''_h_' the magnetic field.

November 22, 2016, at 01:08 PM by 138.96.200.15 -

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%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E'''_h_ denotes the electric field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E''''_h_' denotes the electric field.

November 22, 2016, at 01:07 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes.'''E''' denotes the electric field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. '''E'''_h_ denotes the electric field.

November 22, 2016, at 01:07 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes.'''E~~_h_~~''' denotes the electric field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes.'''E''' denotes the electric field.

November 22, 2016, at 01:07 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. "E" denotes the electric field.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes.'''E_h_''' denotes the electric field.

November 22, 2016, at 01:06 PM by 138.96.200.15 -

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%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering a simple problem of plane wave propagation in vacuum.

to:

%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering the simple problem of a plane wave propagation in vacuum.A cubic domain is discretized using uniform tetrahedral meshes. "E" denotes the electric field.

November 22, 2016, at 01:05 PM by 138.96.200.15 -

Changed line 12 from:

%lfloat text-align=center width=~~250px~~% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg |

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%lfloat text-align=center width=450px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg | HDG method for the three-dimensional frequency-domain Maxwell equations. Numerical convergence analysis considering a simple problem of plane wave propagation in vacuum.

November 22, 2016, at 01:03 PM by 138.96.200.15 -

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(:linebreaks:)

%lfloat text-align=center width=250px% http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg |

June 14, 2016, at 02:31 PM by 138.96.200.15 -

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!!! HORSE -

to:

!!! HORSE - High Order solver for Radar cross Section Evaluation

June 14, 2016, at 02:30 PM by 138.96.200.15 -

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(:linebreaks:)

to:

(:linebreaks:)

HORSE is a simulation software whose development has started in October 2014 in the context of the %newwin% [[http://www-sop.inria.fr/nachos/projects/tecser | ANR TECSER project]]. HORSE is based on a high order HDG method formulated on unstructured tetrahedral and hybrid structured/unstructured (cubic/tetrahedral) meshes for solving the 3D system of frequency-domain Maxwell equations.

June 14, 2016, at 02:29 PM by 138.96.200.15 -

Added lines 1-6:

(:linebreaks:)

!!! HORSE -

(:linebreaks:)
(:linebreaks:)

HORSE

Software.HORSE History