Field Velocity and Mass Renormalization in Classical Electromagnetism

@misc{sebens2026field,
  title = {{Field Velocity and Mass Renormalization in Classical Electromagnetism}},
  author = {Charles T. Sebens},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.23788},
  eprint = {2609.23788},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.23788},
}

TY  - UNPB
TI  - Field Velocity and Mass Renormalization in Classical Electromagnetism
AU  - Charles T. Sebens
PY  - 2026
DA  - 2026/09/20
PB  - arXiv
DO  - 10.48550/arxiv.2609.23788
UR  - https://arxiv.org/abs/2609.23788
AB  - The intricate procedure of mass renormalization in quantum field theory has a simpler precursor in classical electromagnetism. There, the renormalized mass of a charged body includes both its bare mass and its electromagnetic mass. For a body moving at constant low velocity, the electromagnetic mass can be calculated either from the total momentum of the electromagnetic field or from the total energy of the electromagnetic field in the body's rest frame. For a spherically symmetric charge distribution, these methods appear to disagree by a factor of 4/3. This 4/3 problem has a long history. Here, we see that the concept of field velocity can be used to quickly resolve the 4/3 problem. The two methods for finding the electromagnetic mass agree after noting that the average velocity of energy flow in the electromagnetic field is 4/3 the velocity of the body. The energy in the electromagnetic field moves faster than the charged body because, in addition to moving with the body, the field energy must make its way from the back of the body (where it is being emitted) to the front (where it is being absorbed).
ER  -