## Classical Electrodynamics |

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Page ix

And even after almost 60 years, classical electrodynamics still impresses and

delights as a beautiful

transformations. The special theory of relativity is discussed in Chapter 11, where

...

And even after almost 60 years, classical electrodynamics still impresses and

delights as a beautiful

**example**of the covariance of physical laws under Lorentztransformations. The special theory of relativity is discussed in Chapter 11, where

...

Page 93

See, for

SUGGESTED READING The mathematical apparatus and special functions

needed for the solution of potential problems in spherical, cylindrical, spheroidal,

and ...

See, for

**example**, Smythe, pp. 111, 156, or Jeans, p. 244. REFERENCES ANDSUGGESTED READING The mathematical apparatus and special functions

needed for the solution of potential problems in spherical, cylindrical, spheroidal,

and ...

Page 400

135.0(1.072) = 144.7 Mev As another

proton-antiproton pair in proton-proton collisions: p + p → p + p + p + p The mass

difference is AM = 2m, = 1.877 Bev. From (12.41) we find ...

135.0(1.072) = 144.7 Mev As another

**example**consider the production of aproton-antiproton pair in proton-proton collisions: p + p → p + p + p + p The mass

difference is AM = 2m, = 1.877 Bev. From (12.41) we find ...

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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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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge 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 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