Chapter
1.2.4. Example 1: Point Charge
1.2.5. Example 2: Uniformly Charged Sphere
1.3. Ampère-Maxwell’s Law in Differential Form
1.3.1. Circulation and Curl
1.3.2. The Curl and Ampère-Maxwell’s Law
1.3.3. A Compact Differential Form for Ampère-Maxwell’s Law
1.3.4. Example: Magnetic Field of a Current-Carrying Long Straight Wire
1.4. Faraday’s Law in Differential Form
1.5. Some Concluding Remarks
Appendix 1.1: Gauss’s Law in Dielectrics
Appendix 1.2: Ampère-Maxwell’s Law in Magnetic Materials
Historical Note: The Creative Process in Physics. Maxwell and His Equations
Chapter 2: Electromagnetic Waves in Free Space
2.1. Plane Electromagnetic Waves
2.1.1. Maxwell’s Equations in the Absence of Electric Charges and Currents
2.1.2. Transverse Character of Electromagnetic Waves
2.1.3. Derivation of the Wave Equation
2.1.4. Harmonic Plane Waves
2.2. Energy of Electromagnetic Waves
2.2.2. Energy Flux of an Electromagnetic Wave
2.2.3. Intensity of a Harmonic Electromagnetic Wave
Historical Note: Electromagnetic Theory, Oliver Heaviside and the Invention of Vector Analysis
Chapter 3: Guided Electromagnetic Waves
3.2. The Parallel-Plate Waveguide: TE Modes
3.2.1. A Boundary Condition for the Electric Field
3.2.2. Electric Field in TE Modes
3.2.3. Dispersion Relation and Cutoff Frequencies
3.2.4. The Magnetic Field and the Poynting Vector
3.2.5. Phase Velocity and Group Velocity
3.3. The Parallel-Plate Waveguide: TM and TEM Modes
3.3.1. A Boundary Condition for the Magnetic Field
3.3.2. Fields and Cutoff Frequencies in TM Modes
3.4. Rectangular Waveguide: TE Modes
3.4.2. Cutoff Frequencies and Dispersion Relation
3.5. Rectangular Waveguide. TM Modes
3.5.1. Another Boundary Condition for the Magnetic Field
3.5.2. Deriving the Fields and the Cutoff Frequencies
3.5.3. Do TEM Modes Propagate Along a Rectangular Waveguide?
Appendix 3.1: Wave Equation in Several Dimensions
Historical Note: The Beginning of Telecommunications and the Discovery of the Largest Waveguide in the World