## Classical Electrodynamics |

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Page 135

5.2 carrying a current I can be seen to be directed along the normal to the plane

containing the wire and the observation point, so that the lines of

IR | * dl ...

5.2 carrying a current I can be seen to be directed along the normal to the plane

containing the wire and the observation point, so that the lines of

**magnetic****induction**are concentric circles around the wire. The magnitude of B is given byIR | * dl ...

Page 167

John David Jackson. (a) Show that for z > 0 the

calculated by replacing the medium of permeability u by an image current

distribution, J*, with components, pu – 1 pu – 1 At – 1 ...

John David Jackson. (a) Show that for z > 0 the

**magnetic induction**can becalculated by replacing the medium of permeability u by an image current

distribution, J*, with components, pu – 1 pu – 1 At – 1 ...

Page 633

... 108 Magnet, permanent, 161, 167 Magnetic dipole, see Dipole fields, Dipole

moment Magnetic field H, boundary conditions on, 154 definition of macroscopic,

153 see also

... 108 Magnet, permanent, 161, 167 Magnetic dipole, see Dipole fields, Dipole

moment Magnetic field H, boundary conditions on, 154 definition of macroscopic,

153 see also

**Magnetic induction**Magnetic flux density, see**Magnetic induction**...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

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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