Show that $\Delta E / E,$ the fractional loss of energy of a photon during a collision with a particle of mass $m,$ is given by
$$
\frac{\Delta E}{E}=\frac{h f^{\prime}}{m c^{2}}(1-\cos \phi)
$$
where $E$ is the energy of the incident photon, $f^{\prime}$ is the frequency of
the scattered photon, and $\phi$ is defined as in Fig. $38-5 .$