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008 220601s2013 sz | s |||| 0|eng d
020 _a9783031017155
024 7 _a10.1007/978-3-031-01715-5
_2doi
040 _aES-MaUEC
_bspa
_cES-MaUEC
_dES-MaUEC
050 4 _aQC760.4.M37
_b2013 EB
100 1 _aAlkan, Erdogan,
_d1978-
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686826
245 1 0 _aDouble-Grid Finite-Difference Frequency-Domain (DG-FDFD) Method for Scattering from Chiral Objects
_cby Erdogan Alkan, Veysel Demir, Atef Elsherbeni, Ercument Arvas
250 _a1st edition 2013
264 1 _aCham
_bSpringer International Publishing
_c2013
300 _a1 recurso en línea (X, 119 páginas)
336 _atexto
_btxt
_2rdacontent
337 _aelectrónico
_bc
_2rdamedia
338 _arecurso electrónico
_bcr
_2rdacarrier
347 _aarchivo de texto
_bPDF
490 0 _aSynthesis Lectures on Computational Electromagnetics
_x1932-1716
505 0 _aIntroduction -- Chiral Media -- Basics of the Finite-Difference Frequency-Domain (FDFD) Method -- The Double-Grid Finite-Difference Frequency-Domain (DG-FDFD) Method for Bianisotropic Medium -- Scattering FromThree Dimensional Chiral Structures -- ImprovingTime and Memory Efficiencies of FDFD Methods -- Conclusions -- Appendix A: Notations -- Appendix B: Near to Far FieldTransformation.
520 _aThis book presents the application of the overlapping grids approach to solve chiral material problems using the FDFD method. Due to the two grids being used in the technique, we will name this method as Double-Grid Finite Difference Frequency-Domain (DG-FDFD) method. As a result of this new approach the electric and magnetic field components are defined at every node in the computation space. Thus, there is no need to perform averaging during the calculations as in the aforementioned FDFD technique [16]. We formulate general 3D frequency-domain numerical methods based on double-grid (DG-FDFD) approach for general bianisotropic materials. The validity of the derived formulations for different scattering problems has been shown by comparing the obtained results to exact and other solutions obtained using different numerical methods. Table of Contents: Introduction / Chiral Media / Basics of the Finite-Difference Frequency-Domain (FDFD) Method / The Double-Grid Finite-Difference Frequency-Domain (DG-FDFD) Method for Bianisotropic Medium / Scattering FromThree Dimensional Chiral Structures / ImprovingTime and Memory Efficiencies of FDFD Methods / Conclusions / Appendix A: Notations / Appendix B: Near to Far FieldTransformation.
988 _aSynthesis Collection of Technology_2013
650 7 _2embne
_9686825
_aQuiralidad
650 7 _2embne
_9137999
_aElectromagnetismo
_xModelos matemáticos
650 7 _2embne
_9405025
_aAnálisis numérico
700 1 _aDemir, Veysel,
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686819
_d1974-
700 1 _aElsherbeni, Atef Z.
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686708
700 1 _aArvas, Ercument
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686824
776 0 8 _iPrinted edition:
_z9783031005879
776 0 8 _iPrinted edition:
_z9783031028434
856 4 0 _uhttps://go.openathens.net/redirector/universidadeuropea.es?url=https://doi.org/10.1007/978-3-031-01715-5
_zAcceso a este recurso digital (usuarios Universidad Europea de Madrid)
942 _2lcc
_cLE
998 _b02/2023
_dz
_esc
_zSI