| 000 | 03323nam a22005175i 4500 | ||
|---|---|---|---|
| 001 | 978-3-031-01687-5 | ||
| 003 | DE-He213 | ||
| 005 | 20240730164551.0 | ||
| 007 | cr nn 008mamaa | ||
| 008 | 220601s2005 sz | s |||| 0|eng d | ||
| 020 |
_a9783031016875 _9978-3-031-01687-5 |
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| 024 | 7 |
_a10.1007/978-3-031-01687-5 _2doi |
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| 050 | 4 | _aT1-995 | |
| 072 | 7 |
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| 100 | 1 |
_aBushyager, Nathan. _eauthor. _4aut _4http://id.loc.gov/vocabulary/relators/aut _985195 |
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| 245 | 1 | 0 |
_aMRTD (Multi Resolution Time Domain) Method in Electromagnetics _h[electronic resource] / _cby Nathan Bushyager, Manos M. Tentzeris. |
| 250 | _a1st ed. 2005. | ||
| 264 | 1 |
_aCham : _bSpringer International Publishing : _bImprint: Springer, _c2005. |
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| 300 |
_aVII, 108 p. _bonline resource. |
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| 336 |
_atext _btxt _2rdacontent |
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| 337 |
_acomputer _bc _2rdamedia |
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| 338 |
_aonline resource _bcr _2rdacarrier |
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| 347 |
_atext file _bPDF _2rda |
||
| 490 | 1 |
_aSynthesis Lectures on Computational Electromagnetics, _x1932-1716 |
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| 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. | ||
| 650 | 0 |
_aEngineering. _99405 |
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| 650 | 0 |
_aElectrical engineering. _985196 |
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| 650 | 0 |
_aTelecommunication. _910437 |
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| 650 | 1 | 4 |
_aTechnology and Engineering. _985198 |
| 650 | 2 | 4 |
_aElectrical and Electronic Engineering. _985199 |
| 650 | 2 | 4 |
_aMicrowaves, RF Engineering and Optical Communications. _931630 |
| 700 | 1 |
_aTentzeris, Manos M. _eauthor. _4aut _4http://id.loc.gov/vocabulary/relators/aut _985201 |
|
| 710 | 2 |
_aSpringerLink (Online service) _985205 |
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| 773 | 0 | _tSpringer Nature eBook | |
| 776 | 0 | 8 |
_iPrinted edition: _z9783031005596 |
| 776 | 0 | 8 |
_iPrinted edition: _z9783031028151 |
| 830 | 0 |
_aSynthesis Lectures on Computational Electromagnetics, _x1932-1716 _985207 |
|
| 856 | 4 | 0 | _uhttps://doi.org/10.1007/978-3-031-01687-5 |
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| 942 | _cEBK | ||
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