{
  "annotation_id": "c0dbccd2-b6d2-4597-99cb-3edcc2c9da46",
  "date_created": "2026-03-02T18:00:39.822000Z",
  "date_modified": "2026-03-02T18:00:39.822000Z",
  "file_hash": "c4991c0f27dacde5c56d6b695739165ff42a22b142975b8646f305076c6103b5",
  "private": false,
  "record": {
    "abstract": "The appearance of the time derivative of the acceleration in the equation of\nmotion (EOM) of an electric charge is studied. It is shown that when an\nelectric charge is accelerated, a stress force exists in the curved electric\nfield of the accelerated charge, and this force is proportional to the\nacceleration. This stress force acts as a reaction force which is responsible\nfor the creation of the radiation (instead of the \"radiation reaction force\"\nthat actually does not exist at low velocities). Thus the initial acceleration\nshould be supplied as an initial condition for the solution of the EOM of an\nelectric charge. It is also shown that in certain cases, like periodic motions\nof an electric charge, the term that includes the time derivative of the\nacceleration, represents the stress reaction force.",
    "arxiv_id": "physics/0209090",
    "authors": [
      "Amos Harpaz",
      "Noam Soker"
    ],
    "categories": [
      "physics.class-ph"
    ],
    "doi": "10.1023/A:1025627024534",
    "title": "Equation of Motion of an Electric Charge",
    "url": "https://arxiv.org/abs/physics/0209090"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "13fd64e9-c874-47db-b72c-e18396f89689",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}