A short-range, charge-independent force, the nuclear force, is characterized by its dependence solely on the distance between nucleons, irrespective of their charge. Consequently, the strength of the nuclear force between two protons (\( F_{pp} \)), a proton and a neutron (\( F_{pn} \)), and two neutrons (\( F_{nn} \)) is roughly equivalent at close distances within the nucleus. This leads to the equation:
\[
F_{pp} = F_{pn} = F_{nn}
\]