## Classical Electrodynamics |

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Page 463

13.2 13.3 13.4 (a) Takingh(o) = 12Zevin the quantum-mechanicalenergy-loss

formula,

copper, lead for a proton and a mu meson, each with kinetic energies of 10, 100,

1000 ...

13.2 13.3 13.4 (a) Takingh(o) = 12Zevin the quantum-mechanicalenergy-loss

formula,

**calculate**the rate of energy loss (in Mevlcm) in air at NTP, aluminum,copper, lead for a proton and a mu meson, each with kinetic energies of 10, 100,

1000 ...

Page 575

Keeping only lowest-order terms in B and making the long-wavelength

approximation,

distribution of radiation, and the total power radiated. The uniform charge density

of Problem ...

Keeping only lowest-order terms in B and making the long-wavelength

approximation,

**calculate**the nonvanishing multipole moments, the angulardistribution of radiation, and the total power radiated. The uniform charge density

of Problem ...

Page 576

to the energy in the field. ... to perform some integrations by parts, and to use the

differential equation satisfied by E., in order to simplify your

**Calculate**the ratio of the z component of the electromagnetic angular momentumto the energy in the field. ... to perform some integrations by parts, and to use the

differential equation satisfied by E., in order to simplify your

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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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 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