The good thing about,
\(\cfrac{m_e f_e^3}{m_p f_p^3}=\cfrac{r_p^4}{r_e^4}\)
from the previous post "And They Danced" dated 18 Jul 2016, is that the presence of \(\cfrac{f_e^3}{f_p^3}\) allows for the possibility of,
\(\cfrac{1}{77}\lt\cfrac{m_e}{m_p}\le1\)
where an electron in orbit around a nucleus is a basic particle or a group of basic particles of number \(n\lt77\). Such particles coalesce into big particles \(n=77\), on being ejected from the nucleus. If this is the case, an electron beam from cathode ray tube will initially convergence and would need time to coalesce before it has momentum to turn a wind wheel or paddle wheel.
But \(r_p\), the radius of the hydrogen nucleus orbit/spin is not available for a hydrogen nucleus. The common notion is that the hydrogen nucleus is stationary without spin and the electron in orbit around it.
No spin, No show.
