I know this is a classical system, and thus not compliant with the quantum nature of real atoms. But please bare with me.
I have heard this before: the orbiting electron should radiate in the classical Bohr atomic model (point-charge electron and point charge proton orbiting common center of mass).
When searching around, I found it in wikipedia and also in a very popular question and answer here.
Yet I can't see how. I have been checking the literature:
Using Lorentz Force where we account for both the electrical and magnetic fields $\textbf{F}_L = e\textbf{E} + e\textbf{v} \times \textbf{B}$ you find it radiates only if you fix the position of the proton.
If you are committed to be accurate, and work on the center of mass, then magnetic field terms cancel and only electric fields remain. This then leads to classical movement in central field where momentum conservation prevents the electron from falling into the nucleus.
Now for a more serious consideration,
Using Pointing Theorem and then trying to find the radiated energy coming out of the system, with a bit more work, I find that there is nothing coming out. Which is consistent with above, but inconsistent with calculations of radiation coming from an equivalent system: rotating dipole
Where is the mistake?