(a) Shell is fired with velocity $v$ at an angle $\theta$ with the horizontal
So its velocity at the highest point
= horizontal component of velocity $= v\cos\theta$
So momentum of shell before explosion $= mv\cos\theta$
When it breaks into two equal pieces one piece retraces its path to the canon, then other part moves with velocity $V$
So momentum of two pieces after explosion
$= \frac{m}{2}\ \left( - v\cos\theta \right) + \frac{m}{2}V$
By the law of conservation of momentum
$mv\cos\theta = \frac{- m}{2}\ v\cos\theta + \frac{m}{2}\ V \Rightarrow V = 3v\cos\theta$