## Classical Electrodynamics |

### From inside the book

Results 1-3 of 51

Page 19

... in (1.42)

conditions we must be more careful. ... fox) 0GN (x, x') = 0 for x' on S 0n' since that

makes the second term in the surface integral in (1.42)

... in (1.42)

**vanishes**and the solution is on da (144) on' - For Neumann boundaryconditions we must be more careful. ... fox) 0GN (x, x') = 0 for x' on S 0n' since that

makes the second term in the surface integral in (1.42)

**vanish**, as desired.Page 282

(9.64) With this condition on p it can readily be seen that the integral in (9.63)

over the hemisphere S,

radius goes to infinity. Then we obtain the Kirchhoff integral for p(x) in region II: ...

(9.64) With this condition on p it can readily be seen that the integral in (9.63)

over the hemisphere S,

**vanishes**inversely as the hemisphere radius as thatradius goes to infinity. Then we obtain the Kirchhoff integral for p(x) in region II: ...

Page 284

(GE)] doz (9.74) y From the expansion, V × V x A = V(V. A.) – W*A, it is evident

that the volume integral

three terms in (9.72) identically zero, the remaining three terms give an

alternative ...

(GE)] doz (9.74) y From the expansion, V × V x A = V(V. A.) – W*A, it is evident

that the volume integral

**vanishes**identically.* With the surface integral of the firstthree terms in (9.72) identically zero, the remaining three terms give an

alternative ...

### What people are saying - Write a review

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

### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 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 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