Perfectly Matched Layer (PML) for Computational Electromagnetics (Record no. 85789)

000 -LEADER
fixed length control field 03541nam a22005055i 4500
001 - CONTROL NUMBER
control field 978-3-031-01696-7
005 - DATE AND TIME OF LATEST TRANSACTION
control field 20240730164604.0
008 - FIXED-LENGTH DATA ELEMENTS--GENERAL INFORMATION
fixed length control field 220601s2007 sz | s |||| 0|eng d
020 ## - INTERNATIONAL STANDARD BOOK NUMBER
ISBN 9783031016967
-- 978-3-031-01696-7
082 04 - CLASSIFICATION NUMBER
Call Number 620
100 1# - AUTHOR NAME
Author Bérenger, Jean-Pierre.
245 10 - TITLE STATEMENT
Title Perfectly Matched Layer (PML) for Computational Electromagnetics
250 ## - EDITION STATEMENT
Edition statement 1st ed. 2007.
300 ## - PHYSICAL DESCRIPTION
Number of Pages VII, 117 p.
490 1# - SERIES STATEMENT
Series statement Synthesis Lectures on Computational Electromagnetics,
505 0# - FORMATTED CONTENTS NOTE
Remark 2 Introduction -- 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 ## - SUMMARY, ETC.
Summary, etc This 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.
856 40 - ELECTRONIC LOCATION AND ACCESS
Uniform Resource Identifier https://doi.org/10.1007/978-3-031-01696-7
942 ## - ADDED ENTRY ELEMENTS (KOHA)
Koha item type eBooks
264 #1 -
-- Cham :
-- Springer International Publishing :
-- Imprint: Springer,
-- 2007.
336 ## -
-- text
-- txt
-- rdacontent
337 ## -
-- computer
-- c
-- rdamedia
338 ## -
-- online resource
-- cr
-- rdacarrier
347 ## -
-- text file
-- PDF
-- rda
650 #0 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Engineering.
650 #0 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Electrical engineering.
650 #0 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Telecommunication.
650 14 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Technology and Engineering.
650 24 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Electrical and Electronic Engineering.
650 24 - SUBJECT ADDED ENTRY--SUBJECT 1
-- Microwaves, RF Engineering and Optical Communications.
830 #0 - SERIES ADDED ENTRY--UNIFORM TITLE
-- 1932-1716
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-- ZDB-2-SXSC

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