## Classical ElectrodynamicsProblems after each chapter |

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Page 447

We will content ourselves with the extreme relativistic

... can approximate the Bessel functions by their small argument

Then in the relativistic

...

We will content ourselves with the extreme relativistic

**limit**( ß – 1 ) . Furthermore... can approximate the Bessel functions by their small argument

**limits**( 3.103 ) .Then in the relativistic

**limit**the Fermi expression ( 13.70 ) is dE 2 ( ze ) ? Re dx / b...

Page 493

angles such that 2ka sin 1 ( 14.112 ) 2 If the frequency is low enough so that ka <

1 , then the

there will be a region of forward angles less than 1 0 . ( 14.113 ) ka where the ...

angles such that 2ka sin 1 ( 14.112 ) 2 If the frequency is low enough so that ka <

1 , then the

**limit**qa < 1 will apply at all angles . But for frequencies where ka > 1 ,there will be a region of forward angles less than 1 0 . ( 14.113 ) ka where the ...

Page 518

15.5 Radiation cross section in the complete screening

is the semiclassical result . The curve marked “ Bethe - Heitler " is the

quantummechanical Born approximation . 0 wmax For extremely relativistic

particles the ...

15.5 Radiation cross section in the complete screening

**limit**. The constant valueis the semiclassical result . The curve marked “ Bethe - Heitler " is the

quantummechanical Born approximation . 0 wmax For extremely relativistic

particles 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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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical coefficients 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written