(b) For equilibrium of the system torques on $M_{1}$ and $M_{2}$ due to $B_{H}$ must counter balance each other, $i.e.,\ M_{1} \times B_{H} = M_{2} \times B_{H}$. If $\theta$ is the angle between $M_{1}$ and $B_{H}$, then angle between $M_{2}$ and $B_{H}$ will be $(90 - \theta)$; so $M_{1}B_{H}\sin\theta = M_{2}B_{H}\sin{(90 - \theta)}$
$\Rightarrow \tan\theta = \frac{M_{2}}{M_{1}} = \frac{M}{3M} = \frac{1}{3} \Rightarrow \theta = \tan^{- 1}\left( \frac{1}{3} \right)$