Classical Electromagnetism
Classical Electromagnetism Richard Fitzpatrick Professor of Physics The University of Texas at Austin Contents 1 Maxwell's equations 7. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7. Maxwell's equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7. Scalar and Vector Potentials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8. Dirac Delta Function . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9. Three-Dimensional Dirac Delta Function . . . . . . . . . . . . . . . . . . . . . . 9. Solution of Inhomogeneous Wave Equation . . . . . . . . . . . . . . . . . . . . . 10. Retarded Potentials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 16. Retarded Fields.
8 CLASSICAL ELECTROMAGNETISM In integral form, making use of the divergence theorem, this equation becomes d dt V ρdV + S j·dS =0, (1.8) where V is a fixed volume bounded by a surface S.The volume integral represents the net electric
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