(a) When sources are coherent
$I_{R} = I_{1} + I_{2} + 2\sqrt{I_{1}I_{2}}\cos\phi$
At middle point of the screen, $\phi = 0{^\circ}$
$I_{R} = I + I + 2\sqrt{II}\cos{0{^\circ} = 4I}$
When sources are incoherent,
$I_{R}^{'} = I_{1} + I_{2} = I + I + 2I$
$\frac{I_{R}}{I_{R}^{'}} = \frac{4I}{2I} = 2$