Nonradiation condition
Classical nonradiation conditions define the conditions according to
Fourier components synchronous with waves traveling at the speed of light.[2]
History
Finding a nonradiating model for the
Schrödinger's equation
.
In the meantime, our understanding of classical nonradiation has been considerably advanced since 1925. Beginning as early as 1933, fundamental particles. Goedecke was led by his discovery to speculate:[6]
Naturally, it is very tempting to hypothesize from this that the existence of
Planck's constantis implied by classical electromagnetic theory augmented by the conditions of no radiation. Such a hypothesis would be essentially equivalent to suggesting a 'theory of nature' in which all stable particles (or aggregates) are merely nonradiating charge-current distributions whose mechanical properties are electromagnetic in origin.
The nonradiation condition went largely ignored for many years.
point charge in uniform motion, then there is no radiation. Haus uses his formulation to explain Cherenkov radiation
in which the speed of light of the surrounding medium is less than c.
Applications
- The nonradiation condition is important to the study of invisibility physics.[citation needed]
See also
Notes
- S2CID 121169154.
- ^ doi:10.1119/1.14729.
- ^ Ehrenfest, Paul (1910). "Ungleichförmige Elektrizitätsbewegungen ohne Magnet- und Strahlungsfeld". Physikalische Zeitschrift. 11: 708–709.
- .
- "Invisibility Physics: Schott's radiationless orbits". Skulls in the Stars. June 19, 2008.
- .
- .
- ISBN 978-1-4757-0652-9.
- OSTI 1447538.