2015 IEEE Electrical Design of Advanced Packaging and Systems Symposium (EDAPS) 2015
DOI: 10.1109/edaps.2015.7383694
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Acceleration of large electromagnetic simulation including non-orthogonally aligned thin structures by using multi-GPU HIE/C-FDTD method

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Cited by 4 publications
(3 citation statements)
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“…Traditional EMT simulation is limited by the computing power of the simulation platform and the parallel structure of the simulation algorithm. However, in recent years, with the emergence of high-performance computing platforms, EMT simulation platforms have developed from single computer to computer cluster [4], from multi-core CPU [5] to GPU-based [6,7] or FPGA-based [8] heterogeneous computing. The development of the simulation platforms greatly improves the calculation speed of the model and the simulation efficiency of the power systems.…”
Section: Introductionmentioning
confidence: 99%
“…Traditional EMT simulation is limited by the computing power of the simulation platform and the parallel structure of the simulation algorithm. However, in recent years, with the emergence of high-performance computing platforms, EMT simulation platforms have developed from single computer to computer cluster [4], from multi-core CPU [5] to GPU-based [6,7] or FPGA-based [8] heterogeneous computing. The development of the simulation platforms greatly improves the calculation speed of the model and the simulation efficiency of the power systems.…”
Section: Introductionmentioning
confidence: 99%
“…Otros trabajos se centran en CPUs y GPUs que colaboran para resolver distintas partes del dominio de simulación de forma concurrente [7], y también se implementan entornos de cluster multi-GPU para conseguir mayor velocidad e investigar numéricamente el rendimiento [8], [9]. Se encuentran planteamientos MPI (message passing interface) -OpenMP [10]-GPU para calcular RCS con FDTD, que consiguen reducir el tiempo de cálculo de 3dias a 0.8h (RCS de un F-117) [11].…”
Section: Introductionunclassified
“…El campo eléctrico es E=(E x ,E y ,E z ) V/m, y el campo magnético es H=(H x ,H y ,H z ) A/m ,  0 =1/(4π×10 9 ), =4π×10 7 , = r  0, en el aire  r =1, y en el material dieléctrico en el que estan metalizadas nuestras antenas  r =2.65.…”
Section: Introductionunclassified