(a) In a single slit diffraction experiment, position of minima is given by $d\sin\theta = n\lambda$
So for first minima of red $\sin\theta = 1 \times \left( \frac{\lambda_{R}}{d} \right)$
and as first maxima is midway between first and second minima, for wavelength $\lambda$’,
Its position will be
$d{\sin\theta}^{'} = \frac{\lambda^{'} + 2\lambda'}{2} \Rightarrow \sin{\theta'} = \frac{3\lambda^{'}}{2d}$
According to given condition $\sin\theta = \sin\theta'$
$\Rightarrow \lambda^{'} = \frac{2}{3}\lambda_{R}$ so $\lambda^{'} = \frac{2}{3} \times 660 = 440nm = 4400\mathring{\mathrm{A}}$