We are given the work function of the metal, \( \phi_0 = 1.96\,\text{eV} \), and the frequency of the incident light, \( \nu = 6.4 \times 10^{14}\,\text{Hz} \). Instead of working directly in joules, this route first converts the frequency into a wavelength and then uses the handy eV-nanometre form of the photon energy formula.
Step 1: Convert frequency to wavelength.
\[
\lambda = \frac{c}{\nu} = \frac{3 \times 10^{8}}{6.4 \times 10^{14}} = 4.6875 \times 10^{-7}\,\text{m} = 468.75\,\text{nm}
\]
Step 2: Find photon energy directly in eV.
Using the standard shortcut \( E(\text{eV}) = \dfrac{1240}{\lambda(\text{nm})} \), which comes from combining \( hc \) with the eV-joule conversion:
\[
E = \frac{1240}{468.75} \approx 2.65\,\text{eV}
\]
This matches what a direct joule-based calculation would give, confirming the wavelength is computed correctly.
Step 3: Maximum kinetic energy of the photoelectrons.
By Einstein's photoelectric equation, the photon energy splits into the work needed to free the electron and the kinetic energy it carries away:
\[
K_{\max} = E - \phi_0 = 2.65 - 1.96 = 0.69\,\text{eV}
\]
Step 4: Stopping potential.
The stopping potential is the retarding voltage that just brings the fastest photoelectrons to rest, so \( eV_0 = K_{\max} \). Since \( K_{\max} \) is already expressed in eV, the numerical value of \( V_0 \) in volts equals the numerical value of \( K_{\max} \) in eV:
\[
V_0 = 0.69\,\text{V}
\]
So the photon energy is \( 2.65\,\text{eV} \), the maximum kinetic energy of the emitted electrons is \( 0.69\,\text{eV} \), and the stopping potential is \( 0.69\,\text{V} \).
Einstein's Explanation of the Photoelectric Effect:
Einstein explained the 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 hν, where:
The number of photons in a beam of light determines the intensity of the incident light.When a photon strikes a metal surface, it transfers its total energy hν to a free electron in the metal.A part of this energy is used to eject the electron from the metal, and this required energy is called the work function.The remaining energy is carried by the ejected electron as its kinetic energy.