## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 98

Page 9

If the path is closed , the line integral is zero , E dl = 0 ( 1.21 ) $ E . a result that

can also be obtained directly from Coulomb's law . Then application of Stokes's

theorem [ if A ( x ) is a vector field , S is an open

curve ...

If the path is closed , the line integral is zero , E dl = 0 ( 1.21 ) $ E . a result that

can also be obtained directly from Coulomb's law . Then application of Stokes's

theorem [ if A ( x ) is a vector field , S is an open

**surface**, and C is the closedcurve ...

Page 10

The tangential component of electric field can be shown to be continuous across

a boundary

path . It is only necessary to take a rectangular path with negligible ends and one

...

The tangential component of electric field can be shown to be continuous across

a boundary

**surface**by using ( 1.21 ) for the line integral of E around a closedpath . It is only necessary to take a rectangular path with negligible ends and one

...

Page 38

The inversion of the

exception occurs when 0 vanishes on some

the inverted

...

The inversion of the

**surface**S is the**surface**S ' , and vice versa . not . The onlyexception occurs when 0 vanishes on some

**surface**. Then Q ' also vanishes onthe inverted

**surface**. One might think that , since O is arbitrary to the extent of an...

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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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