000			06160cam a2200901Mi 4500
001			ocn830161892
003			OCoLC
005			20230823095423.0
006			m o d
007			cr cnu---unuuu
008			130316s2013 enk ob 001 0 eng d
040			_aEBLCP _beng _epn _cEBLCP _dYDXCP _dDG1 _dOCLCF _dOCLCQ _dOCLCO _dCOO _dDEBSZ _dN$T _dCDX _dIDEBK _dE7B _dUMI _dUKDOC _dDEBBG _dDKDLA _dOCLCQ _dLOA _dDG1 _dOCLCQ
019			_a830512377 _a839305462 _a875001632 _a913841045 _a960200500
020			_a9781118562352 _q(electronic bk.)
020			_a1118562356 _q(electronic bk.)
020			_a1118614003
020			_a9781118614006
020			_a9781118614228 _q(electronic bk.)
020			_a1118614224 _q(electronic bk.)
020			_a9781299314924 _q(MyiLibrary)
020			_a1299314929 _q(MyiLibrary)
020			_z9781118614006
020			_z1118614003
020			_z9781848213913
020			_z1848213913
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029	1		_aCHBIS _b010026694
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029	1		_aDEBBG _bBV041911175
029	1		_aDEBBG _bBV042032031
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029	1		_aNZ1 _b16097844
035			_a(OCoLC)830161892 _z(OCoLC)830512377 _z(OCoLC)839305462 _z(OCoLC)875001632 _z(OCoLC)913841045 _z(OCoLC)960200500
037			_a462742 _bMIL
050		4	_aTK454.4.E5
072		7	_aSCI _x021000 _2bisacsh
072		7	_aSCI _x022000 _2bisacsh
082	0	4	_a537.01515
049			_aMAIN
100	1		_aSaguet, Pierre.
245	1	0	_aNumerical Analysis in Electromagnetics : _bthe TLM Method.
260			_aLondon : _bWiley, _c2013.
300			_a1 online resource (186 pages).
336			_atext _btxt _2rdacontent
337			_acomputer _bc _2rdamedia
338			_aonline resource _bcr _2rdacarrier
490	1		_aISTE
588	0		_aPrint version record.
505	0		_aCover; Numerical Analysis in Electromagnetics; Title Page; Copyright Page; Table of Contents; Introduction; Chapter 1. Basis of the TLM Method: the 2D TLM Method; 1.1. Historical introduction; 1.2. 2D simulation; 1.2.1. Parallel node; 1.2.2. Series node; 1.2.3. Simulation of inhomogeneous media with losses; 1.2.4. Scattering matrices; 1.2.5. Boundary conditions; 1.2.6. Dielectric interface passage conditions; 1.2.7. Dispersion of 2D nodes; 1.3. The TLM process; 1.3.1. Basic algorithm; 1.3.2. Excitation; 1.3.3. Output signal processing; Chapter 2. 3D Nodes; 2.1. Historical development.
505	8		_a2.1.1. Distributed nodes2.1.2. Asymmetrical condensed node (ACN); 2.1.3. The symmetrical condensed node (SCN); 2.1.4. Other types of nodes; 2.2. The generalized condensed node; 2.2.1. General description; 2.2.2. Derivation of 3D TLM nodes; 2.2.3. Scattering matrices; 2.3. Time step; 2.4. Dispersion of 3D nodes; 2.4.1. Theoretical study in simple cases; 2.4.2. Case of inhomogeneous media; 2.5. Absorbing walls; 2.5.1. Matched impedance; 2.5.2. Segmentation techniques; 2.5.3. Perfectly matched layers; 2.5.4. Optimization of the PML layer profile; 2.5.5. Anisotropic and dispersive layers.
505	8		_a2.5.6. Conclusion2.6. Orthogonal curvilinear mesh; 2.6.1. 3D TLM curvilinear cell; 2.6.2. The TLM algorithm; 2.6.3. Scattering matrices for curvilinear nodes; 2.6.4. Stability conditions and the time step; 2.6.5. Validation of the algorithm; 2.7. Non-Cartesian nodes; Chapter 3. Introduction of Discrete Elements and Thin Wires in the TLM Method; 3.1. Introduction of discrete elements; 3.1.1. History of 2D TLM; 3.1.2. 3D TLM; 3.1.3. Application example: modeling of a p-n diode; 3.2. Introduction of thin wires; 3.2.1. Arbitrarily oriented thin wire model.
505	8		_a3.2.2. Validation of the arbitrarily oriented thin wire modelChapter 4. The TLM Method in Matrix Form and the Z Transform; 4.1. Introduction; 4.2. Matrix form of Maxwell's equations; 4.3. Cubic mesh normalized Maxwell's equations; 4.4. The propagation process; 4.5. Wave-matter interaction; 4.6. The normalized parallelepipedic mesh Maxwell's equations; 4.7. Application example: plasma modeling; 4.7.1. Theoretical model; 4.7.2. Validation of the TLM simulation; 4.8. Conclusion; APPENDICES; Appendix A. Development of Maxwell's Equations using the Z Transform with a Variable Mesh.
505	8		_aAppendix B. Treatment of Plasma using the Z Transform for the TLM MethodBibliography; Index.
520			_aThe aim of this book is to give a broad overview of the TLM (Transmission Line Matrix) method, which is one of the "time-domain numerical methods". These methods are reputed for their significant reliance on computer resources. However, they have the advantage of being highly general. The TLM method has acquired a reputation for being a powerful and effective tool by numerous teams and still benefits today from significant theoretical developments. In particular, in recent years, its ability to simulate various situations with excellent precision, including complex materials, has been.
504			_aIncludes bibliographical references (pages 161-169) and index.
650		0	_aElectromagnetism _xMathematical models.
650		0	_aTime-domain analysis.
650		0	_aNumerical analysis.
650		0	_aElectrical engineering _xMathematics.
650		4	_aElectrical engineering _xMathematics.
650		4	_aElectromagnetism _xMathematical models.
650		7	_aSCIENCE _xPhysics _xElectricity. _2bisacsh
650		7	_aSCIENCE _xPhysics _xElectromagnetism. _2bisacsh
650		7	_aElectrical engineering _xMathematics. _2fast _0(OCoLC)fst01728625
650		7	_aElectromagnetism _xMathematical models. _2fast _0(OCoLC)fst00906599
650		7	_aNumerical analysis. _2fast _0(OCoLC)fst01041273
650		7	_aTime-domain analysis. _2fast _0(OCoLC)fst01151183
655		4	_aElectronic books.
776	0	8	_iPrint version: _aSaguet, Pierre. _tNumerical Analysis in Electromagnetics : The TLM Method. _dLondon : Wiley, ©2013 _z9781848213913
830		0	_aISTE.
856	4	0	_uhttp://dx.doi.org/10.1002/9781118562352 _zWiley Online Library
994			_a92 _bDG1
999			_c20319 _d20278
526			_bps