## Classical ElectrodynamicsProblems after each chapter |

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Page 296

The power radiated per unit solid angle in the scalar Kirchhoff

dP dΩ e Pi cos a + cos ( ka ) 2 477 COS a 2J ( kat ) kaξ ( 9.112 ) 2 cos a where P ,

is given by ( 9.104 ) . If we compare the vector Kirchhoff result ( 9.103 ) with ...

The power radiated per unit solid angle in the scalar Kirchhoff

**approximation**isdP dΩ e Pi cos a + cos ( ka ) 2 477 COS a 2J ( kat ) kaξ ( 9.112 ) 2 cos a where P ,

is given by ( 9.104 ) . If we compare the vector Kirchhoff result ( 9.103 ) with ...

Page 297

Then both scalar and vector

ka ) | J ( ka sin 0 ) Pi ( 9.113 ) dΩ ka sin 0 ... There is reason to believe that the

vector Kirchhoff result is close to the correct one , even though the

...

Then both scalar and vector

**approximations**reduce to the common expression , (ka ) | J ( ka sin 0 ) Pi ( 9.113 ) dΩ ka sin 0 ... There is reason to believe that the

vector Kirchhoff result is close to the correct one , even though the

**approximation**...

Page 535

Neglecting the electromagnetic interaction between the two particles , determine

the radiation cross section in the center of mass system for a collision between

these identical particles to the lowest nonvanishing

...

Neglecting the electromagnetic interaction between the two particles , determine

the radiation cross section in the center of mass system for a collision between

these identical particles to the lowest nonvanishing

**approximation**. Show that the...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Wave Guides and Resonant Cavities | 235 |

Copyright | |

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