Consider two atoms of masses $m$ and $m^{\prime}$, bound a distance $R_{0}$ apart and rotating about their center of mass (as in Fig. 12.26). (a) Calculate their moment of inertia, $I$, and prove that it can be written as $I=\mu R_{0}^{2}$, where $\mu$ is the reduced mass
$$
\mu=\frac{m m^{\prime}}{m+m^{\prime}}
$$
This shows that one can treat the rotational motion of any diatomic molecule as if only one of the atoms were moving, provided that one takes its mass to be $\mu$.
(b) Prove that if $m \ll m^{\prime}$, then $\mu \approx \mathrm{m}$.