## Classical ElectrodynamicsProblems after each chapter |

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Page 456

13.7 Mean Square

Scattering Rutherford scattering is confined to very small

Coulomb field , and for fast particles Omax is small compared to unity . Thus there

...

13.7 Mean Square

**Angle**of Scattering and the Angular Distribution of MultipleScattering Rutherford scattering is confined to very small

**angles**even for a pointCoulomb field , and for fast particles Omax is small compared to unity . Thus there

...

Page 458

( O2 ) – 40N In ( 13.111 ) pv The mean square

thickness t . But for reasonable thicknesses such that the particle does not lose

appreciable energy , the Gaussian will still be peaked at very small forward

( O2 ) – 40N In ( 13.111 ) pv The mean square

**angle**increases linearly with thethickness t . But for reasonable thicknesses such that the particle does not lose

appreciable energy , the Gaussian will still be peaked at very small forward

**angles**.Page 459

13.8 Multiple and single scattering distributions of projected

of plural scattering ( a ~ 2–3 ) the dotted curve indicates the smooth transition

from the small -

the ...

13.8 Multiple and single scattering distributions of projected

**angle**. In the regionof plural scattering ( a ~ 2–3 ) the dotted curve indicates the smooth transition

from the small -

**angle**multiple scattering ( approximately Gaussian in shape ) tothe ...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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