Nonrelativistic charge radiation
A nonrelativistic accelerated point charge radiates total power P=q²a²/(6πε₀c³).
Key knowledge
A nonrelativistic accelerated point charge radiates total power P=q²a²/(6πε₀c³). Its far radiation field decreases as 1/r and has the transverse sin²θ angular power pattern relative to the acceleration.
Values and equations
P=q²a²/(6πε₀c³)
- P
- Radiated power W
- q
- Charge C
- a
- Acceleration magnitude m s⁻²
- ε₀
- Vacuum permittivity F m⁻¹
- c
- Vacuum speed of light m s⁻¹
Conditions and scope
- Classical point-charge radiation in vacuum, |v|≪c, acceleration evaluated at retarded time and far-zone radiation separated from near fields.
- Relativistic motion needs the Liénard expression; this does not by itself supply a self-consistent radiation-reaction trajectory or a quantum atomic decay model.
Sources · 1
References
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Evidence and review
Classical Electromagnetism (2014): Larmor formula: Equations 1921–1929: transverse far field, Poynting flux and integrated nonrelativistic power.
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Entry details
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