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999			_c387192 _d387192
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003			ES-MaUEC
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007			cr nn 008mamaa
008			220601s2007 sz | s |||| 0|eng d
020			_a9783031016967
024	7		_a10.1007/978-3-031-01696-7 _2doi
040			_aES-MaUEC _bspa _cES-MaUEC _dES-MaUEC
050		4	_aQC670 _b2007 EB
100	1		_aBérenger, Jean-Pierre _eautor _4aut _4http://id.loc.gov/vocabulary/relators/aut _9686813
245	1	0	_aPerfectly Matched Layer (PML) for Computational Electromagnetics _cby Jean-Pierre Bérenger
250			_a1st edition 2007
264		1	_aCham _bSpringer International Publishing _c2007
300			_a1 recurso en línea (VII, 117 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 -- The Requirements for the Simulation of Free Space and a Review of Existing Absorbing Boundary Conditions -- The Two-Dimensional Perfectly Matched Layer -- Generalizations and Interpretations of the Perfectly Matched Layer -- Time Domain Equations for the PML Medium -- The PML ABC for the FDTD Method -- Optmization of the PML ABC in Wave-Structure Interaction and Waveguide Problems -- Some Extensions of the PML ABC.
520			_aThis lecture presents the perfectly matched layer (PML) absorbing boundary condition (ABC) used to simulate free space when solving the Maxwell equations with such finite methods as the finite difference time domain (FDTD) method or the finite element method. The frequency domain and the time domain equations are derived for the different forms of PML media, namely the split PML, the CPML, the NPML, and the uniaxial PML, in the cases of PMLs matched to isotropic, anisotropic, and dispersive media. The implementation of the PML ABC in the FDTD method is presented in detail. Propagation and reflection of waves in the discretized FDTD space are derived and discussed, with a special emphasis on the problem of evanescent waves. The optimization of the PML ABC is addressed in two typical applications of the FDTD method: first, wave-structure interaction problems, and secondly, waveguide problems. Finally, a review of the literature on the application of the PML ABC to other numerical techniques of electromagnetics and to other partial differential equations of physics is provided. In addition, a software package for computing the actual reflection from a FDTD-PML is provided. It is available here.
988			_aSynthesis Collection of Technology_2007
650		7	_2embne _9686811 _aMaxwell, Ecuaciones de
650		7	_2embne _9145456 _aEcuaciones en derivadas parciales
650		7	_2embne _9139231 _aFísica matemática
776	0	8	_iPrinted edition: _z9783031005688
776	0	8	_iPrinted edition: _z9783031028243
856	4	0	_uhttps://go.openathens.net/redirector/universidadeuropea.es?url=https://doi.org/10.1007/978-3-031-01696-7 _zAcceso a este recurso digital (usuarios Universidad Europea de Madrid)
942			_2lcc _cLE
998			_b02/2023 _dz _esc _zSI