## Classical Electrodynamics |

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Page 91

From (3.170) and an identity of Problem 3.12c this requirement can be seen to

imply lim f(k) = q (3.172) k-0 When boundary conditions (3.171) are applied to the

general solution (3.170), there results a pair of

...

From (3.170) and an identity of Problem 3.12c this requirement can be seen to

imply lim f(k) = q (3.172) k-0 When boundary conditions (3.171) are applied to the

general solution (3.170), there results a pair of

**integral**equations of the first kind:...

Page 284

To do this we make use of the following easily proved identities connecting

surface

three terms in (9.72) identically zero, the remaining three terms give an

alternative ...

To do this we make use of the following easily proved identities connecting

surface

**integrals**over a closed surface S to ... With the surface**integral**of the firstthree terms in (9.72) identically zero, the remaining three terms give an

alternative ...

Page 301

We see that Fon and Fin are proportional to (k+ kg), respectively; the shadow

As the scattering angle departs from the forward direction the shadow

...

We see that Fon and Fin are proportional to (k+ kg), respectively; the shadow

**integral**will be large and the**integral**from the illuminated region will go to zero.As the scattering angle departs from the forward direction the shadow

**integral**will...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

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