| |
| | Electromagnetic Waves (Site not responding. Last check: 2007-10-15) |
 | | The logarithmic potential is infinite not only at the line charge, r → 0, but also at infinity, so we cannot make it vanish there, as we can with the potential of a point charge, that only has a pole at r = 0. |
 | | The logarithmic potential is zero at r = 1, but its absolute value has no significance, and we could add any constant to it that we like without changing the field. |
 | | They resemble the Coulomb dipole fields, but are a quarter-wavelength out of phase and are still considerable at a greater distance than the Coulomb fields. |
| www.du.edu /~jcalvert/phys/emwaves.htm (9513 words) |
|