Faraday’s Law and Induction

  • Nathan Ida


In the previous chapters, we found it useful to treat the electric and magnetic phenomena separately. In Chapters 4 through 7, we treated electrostatic fields by relying on the two postulates:
$$ \left( {\nabla \times E = 0 and \nabla \cdot D = \rho } \right){\text{ or }}\left( {\oint_C {H \cdot d1 = I } {\text{and }}\oint_s B \cdot ds = 0} \right) $$


Magnetic Field Flux Density Electromotive Force Electric Field Intensity Ideal Transformer 
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Copyright information

© Springer Science+Business Media New York 2000

Authors and Affiliations

  • Nathan Ida
    • 1
  1. 1.Department of Electrical EngineeringThe University of AkronAkronUSA

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