According to Einstein’s photoelectric equation:
\[ K_{\text{max}} = h (\nu - \nu_0) \]
Where \( K_{\text{max}} \) is the maximum kinetic energy of the photoelectrons.
The kinetic energy of the photoelectrons is related to the cut-off potential \( V_{\text{cut-off}} \) by:
\[ K_{\text{max}} = eV_{\text{cut-off}} \]
Therefore, we can write:
\[ eV_{\text{cut-off}} = h (\nu - \nu_0) \]
Substituting the given values:
\[ V_{\text{cut-off}} = \frac{h (\nu - \nu_0)}{e} \]
Substitute \( h = 6.63 \times 10^{-34} \, \text{J} \cdot \text{s} \), \( e = 1.6 \times 10^{-19} \, \text{C} \), \( \nu = 6.8 \times 10^{14} \, \text{Hz} \), and \( \nu_0 = 3.6 \times 10^{14} \, \text{Hz} \):
\[ V_{\text{cut-off}} = \frac{(6.63 \times 10^{-34}) \times (6.8 \times 10^{14} - 3.6 \times 10^{14})}{1.6 \times 10^{-19}} \]
\[ V_{\text{cut-off}} = \frac{6.63 \times 10^{-34} \times 3.2 \times 10^{14}}{1.6 \times 10^{-19}} \]
\[ V_{\text{cut-off}} = \frac{2.12 \times 10^{-19}}{1.6 \times 10^{-19}} = 1.33 \, \text{V} \]
Thus, the cut-off potential for the photoelectrons is \( 1.33 \, \text{V} \).
(a) Draw a plot of frequency \( \nu \) of incident radiations as a function of stopping potential \( V_0 \) for a given photo emissive material. What information can be obtained from the value of the intercept on the stopping potential axis?
(b) Calculate : (i) the momentum and (ii) de Broglie wavelength, of an electron with kinetic energy of \( 80\,\text{eV} \).
Einstein explained photoelectric effect on the basis of Planck's quantum theory, where light travels in the form of small bundles of energy called photons. The energy of each photon is \( h\nu \), where \( \nu \) is the frequency of incident light and \( h \) is Planck's constant. The number of photons in a beam of light determines the intensity of the incident light. A photon incident on a metal surface transfers its total energy \( h\nu \) to a free electron in the metal. A part of this energy is used in ejecting the electron from the metal and is called its work function. The rest of the energy is carried by the ejected electron as its kinetic energy.