Abstract
The electric dipole moment \(\mathbf {p}=-e\mathbf {r}\) rotates in the xy plane with frequency \(\omega _{\scriptscriptstyle \mathrm L}\), which is also the frequency of the emitted radiation.
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Notes
- 1.
Actually it is not strictly necessary for the motion to be periodic, it is sufficient that \({\mathrm{d}{\varvec{v}}^2(t)}{\mathrm{d}t}\) vanishes at the initial and final instants of the time interval considered.
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Macchi, A., Moruzzi, G., Pegoraro, F. (2017). Chapter S-10 Solutions for Chapter 10. In: Problems in Classical Electromagnetism. Springer, Cham. https://doi.org/10.1007/978-3-319-63133-2_23
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DOI: https://doi.org/10.1007/978-3-319-63133-2_23
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