PmWiki | HORSE | History

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

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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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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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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':) http://www-sop.inria.fr/nachos/softs/horse/size_mesh.png

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

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

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(:cell align='center':) 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':) 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 -

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(: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 -

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

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

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

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(:cell align='center':) 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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(: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 -

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

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

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

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(:cellnr align='center':) 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 -

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

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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local sparse direct solver, GMRES accelerated Schwarz algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

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HDG method for the three-dimensional frequency-domain Maxwell equations. Plane wave propagation in vacuum. Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local sparse direct solver, GMRES accelerated Schwarz algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

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(: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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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.

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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 -

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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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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.

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

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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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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 -

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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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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 -

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

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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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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 -

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

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

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(:cellnr align='center':) 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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November 22, 2016, at 05:18 PM by 138.96.200.15 -

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(:cellnr align='center':) 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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November 22, 2016, at 05:17 PM by 138.96.200.15 -

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

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

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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local sparse direct solver, GMRES accelerated Schwarz algorithm with MUMPS as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local sparse direct solver, GMRES accelerated Schwarz algorithm with PaStiX as a local sparse direct solver (referred as Krylov+BiCGStab6 in the figures).

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(:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png (:cellnr align='center':) Schwarz algorithm with MUMPS as a local sparse direct solver

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(:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png (:cellnr align='center':) Schwarz algorithm with PaStiX as a local sparse direct solver

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

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(:cellnr align='center':) MaPHyS algebraic hybrid iterative-direct solver with PaStiX as a local sparse direct solver

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(:cellnr align='center':) MaPHyS algebraic hybrid iterative-direct solver with PaStiX as a local sparse direct solver (:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/F-104_Schwarz+PaStiX.png (:cellnr align='center':) 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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November 22, 2016, at 05:11 PM by 138.96.200.15 -

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

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

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

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

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(:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/F-104View1-P2ScaleP3.png (:cell align='center':) 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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(:table border='0' width='100%' align='center' cellspacing='1px':) (:cellnr align='center':) 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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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local (sparse direct) solver,

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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local sparse direct solver, GMRES accelerated 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 -

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Strong scalability analysis: cluster with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network.

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Strong scalability analysis: 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): MUMPS sparse direct solver, MaPHyS algebraic hybrid iterative-direct solver with MUMPS or PaStiX as a local (sparse direct) solver,

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

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Strong scalability analysis

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Strong scalability analysis: cluster with Intel Xeon Haswell E5-2680@2.5 GHz nodes, 24 cores per node, Infiniband QDR TrueScale 40Gb/s network.

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

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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)

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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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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).

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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 03:24 PM by 138.96.200.15 -

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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 -

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

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(:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png (:cell align='center':) 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':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png (:cell align='center':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P2.png

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

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

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(:cellnr align='center':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P3.png (:cell align='center':) 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':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png (:cell align='center':) http://www-sop.inria.fr/nachos/softs/horse/PW_TimesBest_P1.png (:cellnr align='center':) DGTD method with affine elements

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

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

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(:cellnr align='center':) 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':) 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 -

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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.

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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 -

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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.

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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 -

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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.

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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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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.

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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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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.

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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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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.

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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 -

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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.

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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 -

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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.

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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 -

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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.

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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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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.

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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 -

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http://www-sop.inria.fr/nachos/softs/horse/pw_conv.jpg |

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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:)

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 -

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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:)

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(:linebreaks:)

HORSE is a simulation software whose development has started in October 2014 in the context of the 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 -

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(:linebreaks:)

HORSE -

(:linebreaks:) (:linebreaks:)

HORSE

Software.HORSE History

HORSE -

HORSE - High Order solver for Radar cross Section Evaluation

HORSE -