## Classical Electrodynamics |

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Page 296

Choosing the magnitude of E for p, we have, by straightforward calculation with (

9.95), COS 0 + COS o) J1(kaš) 2 kaš as the scalar equivalent of (9.102). The

power radiated per unit solid angle in the scalar Kirchhoff

) ...

Choosing the magnitude of E for p, we have, by straightforward calculation with (

9.95), COS 0 + COS o) J1(kaš) 2 kaš as the scalar equivalent of (9.102). The

power radiated per unit solid angle in the scalar Kirchhoff

**approximation**is ikr y(x) ...

Page 297

Then both scalar and vector

dP (ka)*|J1(ka sin 6) = ~ P, So- |+}d() T ka ... 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,dP (ka)*|J1(ka sin 6) = ~ P, So- |+}d() T ka ... 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 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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