Electromagnetic Lorenz Fields
| dc.creator | Potter, H. C. | |
| dc.date | 2008-10-07 | |
| dc.date | 2008-12-16 | |
| dc.date.accessioned | 2026-07-07T12:12:37Z | |
| dc.date.available | 2026-07-07T12:12:37Z | |
| dc.description | Gauge transformations are potential transformations that leave only specific Maxwell fields invariant. To reveal more, I develop Lorenz field equations with full Maxwell form for nongauge, sans gauge function, transformations yielding mixed, superposed retarded and outgoing, potentials. The form invariant Lorenz condition is then a charge conservation equivalent. This allows me to define three transformation classes that screen for Lorenz relevance. The nongauge Lorentz conditions add polarization fields which support emergent, light-like rays that convey energy on charge conserving phase points. These localized rays escape discovery in modern Maxwell fields where the polarizations are suppressed by gauge transformations. | |
| dc.description | Layout and content revision | |
| dc.identifier | https://arxiv.org/abs/0810.1172 | |
| dc.identifier | http://arxiv.org/abs/0810.1172 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/210603 | |
| dc.subject | General Physics | |
| dc.title | Electromagnetic Lorenz Fields | |
| dc.type | text |