(a) $\mathbf{v}_{CM} = \frac{m_{1}\mathbf{v}_{1} + m_{2}\mathbf{v}_{2}}{m_{1} + m_{2}} = \frac{\mathbf{v}_{\mathbf{1}} + \mathbf{v}_{2}}{2}$ (as $m_{1} = m_{2}$)
and $\mathbf{a}_{CM} = \frac{m_{1}\mathbf{a}_{1} + m_{2}\mathbf{a}_{2}}{m_{1} + m_{2}}$
$= \frac{\mathbf{a}_{1} + 0}{2} = \frac{\mathbf{a}_{1}}{2}$
The centre of mass of two particles will move with the mean velocity of two particles having common acceleration $\frac{\mathbf{a}}{2}$.
Hence, path of CM will be a straight line.