## Classical Electrodynamics |

### From inside the book

Results 1-3 of 65

Page 166

(b) Show that an alternative

kp) 0 (c) Write down integral

induction, using the

components of B ...

(b) Show that an alternative

**expression**for A4 is oo A4(p, z) = *. dke-ko J1(ka).J1(kp) 0 (c) Write down integral

**expressions**for the components of magneticinduction, using the

**expressions**of (a) and (b). Evaluate explicitly thecomponents of B ...

Page 295

For ka > 1, the second form in (9.109) can be used to obtain an asymptotic

9.109) and (9.110) for T give the general behavior as a function of ka, but are not

very ...

For ka > 1, the second form in (9.109) can be used to obtain an asymptotic

**expression**, 1 1 - ( #) Tcz 1 — — — — —Hz sin 2ka ... approximate**expressions**(9.109) and (9.110) for T give the general behavior as a function of ka, but are not

very ...

Page 447

where we have used the dipole moment

second term is small, the imaginary part of 1/e(0) can be readily calculated and

substituted into (13.70). Then the integral over do can be performed in the same ...

where we have used the dipole moment

**expression**(13.19). Assuming that thesecond term is small, the imaginary part of 1/e(0) can be readily calculated and

substituted into (13.70). Then the integral over do can be performed in the same ...

### What people are saying - Write a review

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

### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

### 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