Question:

When UV light of wavelength 300 nm is incident on the metal surface having work function 2.13 eV, electron emission takes place. The stopping potential is : (Given hc = 1240 eV nm)

Updated On: Nov 3, 2025
  • 4 V
  • 4.1 V
  • 2 V
  • 1.5 V
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The Correct Option is C

Approach Solution - 1

The energy of the incident photon is given by:
\[\frac{hc}{\lambda} = eV_s + \phi\]
Substitute the given values:
\[\frac{1240}{300} \, \text{eV} - 2.13 \, \text{eV} = eV_s\]
\[4.13 \, \text{eV} - 2.13 \, \text{eV} = eV_s\]
\[V_s = 2 \, \text{V}\]

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Approach Solution -2

To find the stopping potential when UV light of wavelength 300 nm is incident on a metal surface with a work function of 2.13 eV, we can use the photoelectric effect equation. According to the photoelectric equation:

\(E_k = h f - \Phi\)

Where:

  • \(E_k\) is the kinetic energy of the emitted electrons.
  • \(h\) is Planck's constant.
  • \(f\) is the frequency of the incident light.
  • \(\Phi\) is the work function of the metal.

The stopping potential \(V_0\) is related to the maximum kinetic energy by:

\(E_k = e V_0\)

Where \(e\) is the charge of an electron (approximately \(1.6 \times 10^{-19}\) coulombs).

First, convert the wavelength to energy using the relation:

\(E = \frac{hc}{\lambda}\)

Given \(hc = 1240 \text{ eV nm}\) and \(\lambda = 300 \text{ nm}\), we have:

\(E = \frac{1240 \text{ eV nm}}{300 \text{ nm}} = 4.13 \text{ eV}\)

Now, substitute this into the photoelectric equation:

\(E_k = E - \Phi = 4.13 \text{ eV} - 2.13 \text{ eV} = 2.00 \text{ eV}\)

Hence, the stopping potential \(V_0\) can be found using:

\(E_k = e V_0\)

\(V_0 = 2.00 \text{ volts}\)

Thus, the stopping potential is 2 V

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