Transcription of Chapter 13 Maxwell’s Equations and Electromagnetic Waves
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Chapter 13 Maxwell’s Equations and Electromagnetic Waves
Chapter 13 Maxwell s Equations and Electromagnetic Waves The Displacement Gauss s Law for Maxwell s Plane Electromagnetic One-Dimensional Wave Standing Electromagnetic Poynting Example : Solar Example : Intensity of a Standing Energy Momentum and Radiation Production of Electromagnetic Animation : Electric Dipole Radiation Animation : Electric Dipole Radiation Animation : Radiation From a Quarter-Wave Plane Sinusoidal Electromagnetic Appendix: Reflection of Electromagnetic Waves at Conducting 13-35 Problem-Solving Strategy: Traveling Electromagnetic Solved Plane Electromagnetic One-Dimensional Wave Poynting Vector of a Charging Poynting Vector of a Conceptual Additional Solar Reflections of True Coaxial Cable and Power Superposition of Electromagnetic Sinusoidal Electromagnetic Radiation Pressure of Electromagnetic Energy of Electromagnetic Wave Electromagnetic Plane Sinusoidal Electromagnetic 13.
magnetic field can be obtained by using Ampere’s law: ∫Bs⋅=dµ0eInc GG v (13.1.1) The equation states that the line integral of a magnetic field around an arbitrary closed loop is equal to µ0eI nc, where Ienc is the conduction current passing through the surface bound by the closed path. In addition, we also learned in Chapter 10 that, as a
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