## Classical ElectrodynamicsProblems after each chapter |

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Page 304

The total power

The total power

**scattered**is obtained by integrating over all angles . ... area of the sphere for**scattering**( its**scattering**cross section ) is 27a .Page

The multiple -

The multiple -

**scattering**distribution for the projected angle of**scattering**is 1 A12 PM ( 0 ' ) de ' = exp do ' ( 13.112 ) 7 ( 02 ) where both positive and ...Page

13.8 Multiple and single

13.8 Multiple and single

**scattering**distributions of projected angle . In the region of plural**scattering**( & ~ 2–3 ) the dotted curve indicates the smooth ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

9 other sections not shown

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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution sphere spherical surface transformation unit vanishes vector velocity volume wave written