Difference between revisions of "Inactive Portion of the Radiative Part of the Li?nard-Wiechert Field"
Jump to navigation
Jump to search
(Imported from text file) |
(Imported from text file) |
||
| (One intermediate revision by the same user not shown) | |||
| Line 16: | Line 16: | ||
==Abstract== | ==Abstract== | ||
| − | A point charge in motion generates the Li?nard-Wiechert energy-momentum tensor. Teitelboim showed that this tensor splits into its bounded part ac B T and its radiative part ac R T . All the terms in ac B Tare know to contribute to the matter-field energy-momentum balance. In this paper the inactive part of ac R T is found, i.e., the terms do not contribute to the energy-momentum fluxes are shown. | + | A point charge in motion generates the Li?nard-Wiechert energy-momentum tensor. Teitelboim showed that this tensor splits into its bounded part ac B T and its radiative part ac R T . All the terms in ac B Tare know to contribute to the matter-field energy-momentum balance. In this paper the inactive part of ac R T is found, i.e., the terms do not contribute to the energy-momentum fluxes are shown. |
| − | [[Category:New Energy]] | + | [[Category:Scientific Paper|inactive portion radiative part li nard-wiechert field]] |
| + | |||
| + | [[Category:New Energy|inactive portion radiative part li nard-wiechert field]] | ||
Latest revision as of 19:38, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Inactive Portion of the Radiative Part of the Li?nard-Wiechert Field |
| Read in full | Link to paper |
| Author(s) | Jose Luis Lopez-Bonilla |
| Keywords | energy-momentum tensor, bounded part, radiative part |
| Published | 2002 |
| Journal | Apeiron |
| Volume | 9 |
| Number | 1 |
| No. of pages | 6 |
| Pages | 43-48 |
Read the full paper here
Abstract
A point charge in motion generates the Li?nard-Wiechert energy-momentum tensor. Teitelboim showed that this tensor splits into its bounded part ac B T and its radiative part ac R T . All the terms in ac B Tare know to contribute to the matter-field energy-momentum balance. In this paper the inactive part of ac R T is found, i.e., the terms do not contribute to the energy-momentum fluxes are shown.
