000 03136nam a22004335i 4500
999 _c387187
_d387187
001 387187
003 ES-MaUEC
005 20230212140919.0
006 a||||fo|||| 00| 0
007 cr nn 008mamaa
008 220601s2005 sz | s |||| 0|eng d
020 _a9783031016875
024 7 _a10.1007/978-3-031-01687-5
_2doi
040 _aES-MaUEC
_bspa
_cES-MaUEC
_dES-MaUEC
050 4 _aQC760.4.M37
_b2005 EB
100 1 _aBushyager, Nathan Adam
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686793
245 1 0 _aMRTD (Multi Resolution Time Domain) Method in Electromagnetics
_cby Nathan Bushyager, Manos Tentzeris
250 _a1st edition 2005
264 1 _aCham
_bSpringer International Publishing
_c2005
300 _a1 recurso en línea (VII, 108 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 -- Background -- Modeling of Practical Structures -- Other Techniques Necessary for Simulation: UPML, Variable Gridding, Source Excitation and Time/Space Adaptive Gridding -- MRTD Simulation Examples.
520 _aThis book presents a method that allows the use of multiresolution principles in a time domain electromagnetic modeling technique that is applicable to general structures. The multiresolution time-domain (MRTD) technique, as it is often called, is presented for general basis functions. Additional techniques that are presented here allow the modeling of complex structures using a subcell representation that permits the modeling discrete electromagnetic effects at individual equivalent grid points. This is accomplished by transforming the application of the effects at individual points in the grid into the wavelet domain. In this work, the MRTD technique is derived for a general wavelet basis using a relatively compact vector notation that both makes the technique easier to understand and illustrates the differences between MRTD basis functions. In addition, techniques such as the uniaxial perfectly matched layer (UPML) for arbitrary wavelet resolution and non-uniform gridding are presented. Using these techniques, any structure that can be simulated in Yee-FDTD can be modeled with in MRTD.
988 _aSynthesis Collection of Technology_2005
650 7 _2embne
_9161271
_aWavelets (Matemáticas)
650 7 _2embne
_9137999
_aElectromagnetismo
_xModelos matemáticos
650 7 _2embne
_9138446
_aAnálisis de sistemas
700 1 _aTentzeris, Manos M.
_eautor
_4aut
_4http://id.loc.gov/vocabulary/relators/aut
_9686223
776 0 8 _iPrinted edition:
_z9783031005596
776 0 8 _iPrinted edition:
_z9783031028151
856 4 0 _uhttps://go.openathens.net/redirector/universidadeuropea.es?url=https://doi.org/10.1007/978-3-031-01687-5
_zAcceso a este recurso digital (usuarios Universidad Europea de Madrid)
942 _2lcc
_cLE
998 _b02/2023
_dz
_esc
_zSI