## Classical Electrodynamics |

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Page 392

For neutral

impossible to obtain their relativistic transformation properties in this ... A charged

For neutral

**particles**with no detectable electromagnetic interactions it is clearlyimpossible to obtain their relativistic transformation properties in this ... A charged

**particle**can be thought of as a very localized distribution of charge and mass.Page 393

The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic

of the

scalar product (12.5) gives the energy of the

The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic

of the

**particle**: 2. (pop). = (p. 2)--. (12.5) In the rest frame of the**particle**(p = 0) thescalar product (12.5) gives the energy of the

**particle**at rest: E' = A (12.6) To ...Page 417

12.7 (a)

induction. (b) Curvature of lines of magnetic induction will cause drift

perpendicular to the (r, y) plane. |VB|B|< 1, the drift velocity is small compared to

the orbital ...

12.7 (a)

**Particle**moving in helical path along lines of uniform, constant magneticinduction. (b) Curvature of lines of magnetic induction will cause drift

perpendicular to the (r, y) plane. |VB|B|< 1, the drift velocity is small compared to

the orbital ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

BoundaryValue Problems in Electrostatics II | 54 |

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 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written