## Classical Electrodynamics |

### From inside the book

Results 1-3 of 99

Page 9

If the path is closed, the line integral is zero, # e.a. = 0 (1.21) a result that can also

be obtained directly from Coulomb's law. Then application of Stokes's theorem [if

A(x) is a vector field, S is an open

If the path is closed, the line integral is zero, # e.a. = 0 (1.21) a result that can also

be obtained directly from Coulomb's law. Then application of Stokes's theorem [if

A(x) is a vector field, S is an open

**surface**, and C is the closed curve bounding ...Page 10

The tangential component of electric field can be shown to be continuous across

a boundary

It is only necessary to take a rectangular path with negligible ends and one side ...

The tangential component of electric field can be shown to be continuous across

a boundary

**surface**by using (1.21) for the line integral of E around a closed path.It is only necessary to take a rectangular path with negligible ends and one side ...

Page 240

0 877 0 16t This is the same rate of energy dissipation as given by the Poynting's

vector result (8.12). The current density J is confined to such a small thickness

just below the

...

0 877 0 16t This is the same rate of energy dissipation as given by the Poynting's

vector result (8.12). The current density J is confined to such a small thickness

just below the

**surface**of the conductor that it is equivalent to an effective**surface**...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

### Other editions - View all

### 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 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