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
consequence of the Faraday’s law of induction, a changing magnetic field can produce an electric field, according to S d d dt ∫Es⋅ =− ∫∫B⋅dA GG GG v (13.1.2) One might then wonder whether or not the converse could be true, namely, a changing electric field produces a magnetic field. If so, then the right-hand side of Eq. (13.1.1) will
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