(a) Einstein’s Photoelectric Equation:
Einstein explained the photoelectric effect using quantum theory.
He proposed that light consists of photons, each with energy:
\[
E = h\nu = \frac{hc}{\lambda}
\]
When a photon strikes a metal surface, it transfers energy to an electron.
If this energy exceeds the work function \( \phi \), the electron is emitted.
Einstein's equation:
\[
h\nu = \phi + K_{\text{max}} \Rightarrow K_{\text{max}} = h\nu - \phi
\]
where:
- \( h \) = Planck’s constant,
- \( \nu \) = frequency of incident light,
- \( \phi \) = work function,
- \( K_{\text{max}} \) = maximum kinetic energy of photoelectrons.
(b) Step-by-step Analysis:
Given:
\[
\lambda = 330\,\text{nm} = 330 \times 10^{-9}\,\text{m}, \quad h = 6.626 \times 10^{-34}, \quad c = 3 \times 10^8
\]
Energy of one photon:
\[
E = \frac{hc}{\lambda} = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{330 \times 10^{-9}} \approx 6.02 \times 10^{-19}\,\text{J}
\]
Convert to eV:
\[
E = \frac{6.02 \times 10^{-19}}{1.6 \times 10^{-19}} \approx 3.76\,\text{eV}
\]
Compare with work functions:
\begin{itemize}
\item K = 2.3 eV less than 3.76 → Emission occurs
\item Na = 2.75 eV less than 3.76 → Emission occurs
\item Mo = 4.17 eV greater than 3.76 → No emission
\item Ni = 5.15 eV greater than 3.76 → No emission
\end{itemize}
Conclusion:
- Metals Mo and Ni will not show photoelectric emission.
Effect of decreasing distance (from 1 m to 0.5 m):
- Intensity increases (since intensity \( \propto \frac{1}{r^2} \)),
- Number of emitted electrons increases (for those metals already emitting),
- \textit{But} photon energy remains the same,
- So Mo and Ni still will not emit electrons (since energy \(<\phi \)).