A Review Of Computational Electromagnetics In China

Zhang, Wen Xun

doi:10.1109/map.1997.598560

Cited by 1 publication

(5 citation statements)

References 26 publications

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“…The equations (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20) and are the homogeneous Helmholtz wave equations for E z and H z , respectively. In order to solve these equations in cylindrical coordinates, the method of separation of variables can be used [55].…”

Section: Source-free Axial Electromagnetic Fieldsmentioning

confidence: 99%

“…A similar procedure was done in [1,11,49]. Setting the wave equations (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19) and (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20) to homogeneous equations and applying (5-22), we obtain…”

Section: Modal Excitation From An Electric Current Sourcementioning

confidence: 99%

“…where k 2 ρ is given by the equation with m(k ρ ) > 0. Also applying the transform (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20)(21)(22) to the source terms in (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19) and (5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18)(19)(20), we obtain…”

Section: Modal Excitation From An Electric Current Sourcementioning

confidence: 99%

“…These methods are usually based on the spatial discretization of Maxwell's equations on the grounds of the finite-difference time-domain method (FDTD) [11,12,13] and the finite element method (FEM) [14,15,16]. Also, other numerical techniques such as the finite volume method (FVM) [17,18], the method of moments (MoM) and the boundary element method (BEM) [19] are also used. Such methods, however, present a high cost in terms of computational time and RAM memory requirements, becoming prohibitive for large problems as well as in iterative solvers.…”

Section: General Introductionmentioning

confidence: 99%

“…19 Normalized amplitude of the azimuthal component of the electric field (E φ ) for decoupled TE and TM modes in a homogeneous and isotropic medium confined by a parallel plate waveguide (Third Mode).…”

mentioning

confidence: 99%

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Study of the Electromagnetic Propagation in Stratified Anisotropic Media via Semi-Analytical Methods

HERNANDEZ¹

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Firstly, I would like to thank to my family, and in a very special way to my parents and my sister for always being present despite the distance. They are my reason I wake up stronger every day and I continue this difficult journey without them. I wish to thank to my husband, Emilio, for being my main support, for walking beside me at all times, for his dedication and unconditional love, simply my best friend. I am very grateful to my advisor, Professor Guilherme Simon da Rosa, for his wisdom and patience, for sharing his knowledge and teaching me tirelessly, for being the light and backbone of this work. This goal would not have been possible without his unconditional guide. It has been a great pleasure working with him. I would like to thank to all my friends and colleagues for supporting me in one or another way, especially to Adila, David, Randy, Julio, Dayrene, Adrián, Reinier, Johnes, Yoiz and Pedro. I want to thank to CETUC and all its professors and workers for giving me a warm welcome and make me feel at home. I would like to thank to PUC-Rio for the exemption of school fees offered by the Programa de Pós-Graduação em Engenharia Elétrica. This study was financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior-Brasil (CAPES)-Finance Code 001.

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