(a) $\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ E = \frac{hc}{\lambda} \Rightarrow E \propto \frac{1}{\lambda}$
$\Rightarrow \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ $ $\ \frac{E^{'}}{E} = \frac{400}{300} = 1.33$
But $E = eV_{s},\ V_{s}$ being stopping potential. Thus, stopping potential for photoelectrons from a surface becomes approximately 1.0 V greater.