Transcription of Chapter 13 Maxwell’s Equations and Electromagnetic Waves
{{id}} {{{paragraph}}}
Example: air traffic controller
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 13-2 Maxwell s Equations and Electromagnetic Waves
bound by the closed path. In addition, we also learned in Chapter 10 that, as a 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
Tags:
Information
Domain:
Source:
Link to this page:
Please notify us if you found a problem with this document: