## Classical Electrodynamics |

### From inside the book

Results 1-3 of 85

Page 24

(c) The electric field at the surface of a conductor is normal to the surface and has

a

infinite, conducting, plane sheets of uniform thicknesses ti and to, respectively, ...

(c) The electric field at the surface of a conductor is normal to the surface and has

a

**magnitude**470, where q is the charge density per unit area on the surface. Twoinfinite, conducting, plane sheets of uniform thicknesses ti and to, respectively, ...

Page 29

When q is just outside the surface of the sphere, the image charge is equal and

opposite in

charge has been found, we can return to the original problem of a charge q

outside a ...

When q is just outside the surface of the sphere, the image charge is equal and

opposite in

**magnitude**and lies just beneath the surface. Now that the imagecharge has been found, we can return to the original problem of a charge q

outside a ...

Page

... (14.27) with the power radiated for acceleration perpendicular to the velocity (

14.46) for the same

force) is ymW.

... (14.27) with the power radiated for acceleration perpendicular to the velocity (

14.46) for the same

**magnitude**of applied force. For circular motion, the**magnitude**of the rate of change of momentum (which is equal to the appliedforce) is ymW.

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User Review - barriboy - LibraryThingA soul crushing technical manual written by a sadist that has served as the right of passage for physics PhDs since the dawn of time. Every single one of my professors studied this book, and every ... Read full review

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### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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### Common terms and phrases

angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written