1 Introduction |
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II.1 Problem Partitioning |
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II.2 Network Representations |
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II.3 Methodological Hybridization |
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III Organization of the Book |
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2 Representations of Electromagnetic Fields |
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II.1 Maxwell's Equations in TimeDependent Form |
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II.2 Maxwell's Equations in the Frequency Domain |
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II.3 Maxwell's Equations in the S-Domain |
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II.4 Constitutive Relations |
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III Theorems and Concepts for Electromagnetic Field Computation |
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III.2 Field Theoretic Formulation of Tellegen's Theorem |
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III.4 Equivalence Theorem |
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V Separation of Variables: The Scalar Wave Equation |
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V.1 The Scalar Wave Equation in Cartesian Coordinates |
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V.2 The Scalar Wave Equation in Spherical and Polar Coordinates |
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V.3 The Scalar Wave Equation in Cylindrical Polar Coordinates |
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VI SturmLiouville Problems |
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VI.1 SourceFree Solutions: Eigenvalue Problem |
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VI.2 Source-Driven Solutions: Green's Function Problem |
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VI.3 Relation Between the Spectral (Characteristic) Green's Function and the Eigenvalue Problems |
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VII Radiation and Edge Condition |
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VII.1 Radiation Condition |
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VII.2 Edge Condition in Two Dimensions |
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VIII Reciprocity and Field Equivalence Principles |
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VIII.1 Reaction in Electromagnetic Theory |
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VIII.2 Lorentz Reciprocity Theorem |
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3 WaveGuiding Configurations |
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II The Transverse Field Equations |
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IV Modal Representations of the Fields and Their Sources |
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V Scalarization and Modal Representation of Dyadic Green's Functions in Uniform Regions |
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VI Fields in Source-Free, Homogeneous Regions |
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VII Green's Functions for the Transmission-Line Equations |
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VIII Modal Representations of the Dyadic Green's Functions in a Piecewise Homogeneous Medium |
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IX Modal Representations of the Dyadic Green's Functions in an Inhomogeneous Medium |
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X NetworkOriented Formulation of the Characteristic Green's Functions |
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X.1 Alternative Representations |
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XI 1D Characteristic Green's Function and Eigenfunction |
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4 TwoDimensional Problems |
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II Electric Line Source in a PEC Parallel Plate Waveguide |
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II.1 Constituent OneDimensional Problems: x-Domain |
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II.2 Problems in the z-Domain |
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II.3 Two-Dimensional Waveguide:(Finite x)-(Bilaterally Infinite z)-Domain |
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III Electric Line Source in Radial-Angular Waveguides |
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III.2 Constituent 1D Problems |
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III.3 Eigenvalue Problem in the p-Domain |
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III.4 Spectral Green's function problem in the p-domain |
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III.5 Two-Dimensional Green's Functions: Alternative Representations |
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5 Network Representation of Electromagnetic Fields |
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III Regions of Zero Volume: the Connection Network |
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III.1 The Connection Network |
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III.2 Tellegen's Theorem for Discretized Fields |
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III.3 Testing of the Field Continuity Equations |
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III.4 Independent Quantities |
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III.5 Tellegen's Theorem and its Implications |
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III.6 Application to Orthonormal Bases |
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III.7 Canonical Forms of the Connection Network |
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IV Network Representations for Regions of Finite Volume |
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IV.1 Foster Representation of the Transmission Line Resonator |
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IV.2 Green's Function and Multiport Foster Representation |
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IV.3 The Canonical Foster Representation of Distributed Circuits |
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V Regions Extending to Infinity: Radiation Problems |
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V.1 The Caner Canonic Representation of Radiation Modes |
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V.2 The Complete Equivalent Circuit of Radiating Electromagnetic Structures |
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VI Solving the Entire Field Problem via Tableau Equations |
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VI.1 Primary and Secondary Fields |
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VI.2 Choice of Primary and Secondary Fields for a Subregion |
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VI.3 A Constraint on the Choice of Primary and Secondary Fields |
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VI.4 Topological Relationships: Operator Form |
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VI.5 The Tableau Equations for Fields: Operator Form |
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VI.6 Solving the Entire Field Problem via Tableau Equations: Discretized Form |
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VI.7 Field Discretization |
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VI.8 The Tableau Equations for Discretized Fields |
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Appendix |
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Index |
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