## Classical Electrodynamics |

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Page 456

7 Mean Square Angle of

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

is a ...

7 Mean Square Angle of

**Scattering**and the Angular Distribution of Multiple**Scattering**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

is a ...

Page 458

But for reasonable thicknesses such that the particle does not lose appreciable

energy , the Gaussian will still be peaked at very small forward angles . The

multiple -

= _ 1 ...

But for reasonable thicknesses such that the particle does not lose appreciable

energy , the Gaussian will still be peaked at very small forward angles . The

multiple -

**scattering**distribution for the projected angle of**scattering**PM ( O ' ) do '= _ 1 ...

Page 459

8 Multiple and single

plural

the small - angle multiple

8 Multiple and single

**scattering**distributions of projected angle . In the region ofplural

**scattering**( a ~ 2 - 3 ) the dotted curve indicates the smooth transition fromthe small - angle multiple

**scattering**( approximately Gaussian in shape ) to the ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

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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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes 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 space sphere spherical surface transformation unit vanishes vector velocity volume wave written