(d) $\frac{hc}{\lambda} = W_{0} + \frac{1}{2}mv_{\max}^{2}$
Assuming $W_{0}$ to be negligible in comparison to $\frac{hc}{\lambda}$
$i.e.\ v_{\max}^{2} \propto \frac{1}{\lambda} \Rightarrow v_{\max} \propto \frac{1}{\sqrt{\lambda}}$
[On increasing wavelength $\lambda$ to $4\lambda,\ v_{\max}$ becomes half]