\( E = \frac{hc}{\lambda} \)
Where \( h \) is Planck’s constant, \( c \) is the speed of light, and \( \lambda \) is the wavelength.
\( E = \frac{(6.626 \times 10^{-34} \, \text{Js}) (3 \times 10^8 \, \text{m/s})}{4770 \times 10^{-10} \, \text{m}} = 4.15 \, \text{eV} \)
Conclusion: Metal D emits electrons because its work function (\( 2.3 \, \text{eV} \)) is less than the photon energy (\( 4.15 \, \text{eV} \)).
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).