## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

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Page 185

The displacement of the poles can be accomplished mathematically by

+ /e) in place of w in (6.59). ... Then G = — dk sin (kR) sin (crk) (6.62) Since the

integrand is even in k, the integral can be

k ...

The displacement of the poles can be accomplished mathematically by

**writing**(w+ /e) in place of w in (6.59). ... Then G = — dk sin (kR) sin (crk) (6.62) Since the

integrand is even in k, the integral can be

**written**over the whole interval, — oo <k ...

Page 384

The Lorentz force equation can be

representing the rate of change of mechanical ...

of f, we find , f '17 i ( J D t D\ f U 7 IFF i IT 7 \ (\\ 1 0"7\ Jl — p**l "T~ ~~ \V2 »i —

Jfl&Z' ...

The Lorentz force equation can be

**written**as^a force per unit volume (representing the rate of change of mechanical ...

**Writing**out a single componentof f, we find , f '17 i ( J D t D\ f U 7 IFF i IT 7 \ (\\ 1 0"7\ Jl — p**l "T~ ~~ \V2 »i —

Jfl&Z' ...

Page 385

(11.129), the force density becomes (11.131) The right-hand side of (1 1.131) can

be

symmetric tensor T^, called the electromagnetic stress-energy-momentum tensor,

...

(11.129), the force density becomes (11.131) The right-hand side of (1 1.131) can

be

**written**as the divergence of a tensor of the second rank. We define thesymmetric tensor T^, called the electromagnetic stress-energy-momentum tensor,

...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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