dorsal/arxiv
View SchemaIntroducing Time Dependence into the Static Maxwell Equations
| Authors | Avraham Gal |
|---|---|
| Categories | |
| ArXiv ID | physics/0106088 |
| URL | https://arxiv.org/abs/physics/0106088 |
Abstract
Using to a minimum extent special relativity input, and relying on the Lorentz-force expression for the force acting on a charged particle in motion under the influence of electric (E) and magnetic (B) fields, the Maxwell curl equations are shown to follow from the covariance of the two Maxwell divergence equations ${\div\cdot E} = 4\pi\rho$ and ${\div\cdot B} = 0$.
{
"annotation_id": "70e2c3a6-c4f1-4799-a5d6-d861c72de14b",
"date_created": "2026-03-02T18:00:35.993000Z",
"date_modified": "2026-03-02T18:00:35.993000Z",
"file_hash": "eaac94828e8f44cc2b32565f5a19d234ba7a9b3156c27460ac3ffe7946386120",
"private": false,
"record": {
"abstract": "Using to a minimum extent special relativity input, and relying on the\nLorentz-force expression for the force acting on a charged particle in motion\nunder the influence of electric (E) and magnetic (B) fields, the Maxwell curl\nequations are shown to follow from the covariance of the two Maxwell divergence\nequations ${\\div\\cdot E} = 4\\pi\\rho$ and ${\\div\\cdot B} = 0$.",
"arxiv_id": "physics/0106088",
"authors": [
"Avraham Gal"
],
"categories": [
"physics.ed-ph"
],
"title": "Introducing Time Dependence into the Static Maxwell Equations",
"url": "https://arxiv.org/abs/physics/0106088"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "9c71e00c-741e-4848-9e4e-27bc20639fef",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}