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Question: When a metallic surface is illuminated with light of wavelength \(\lambda \), the stopping potential...

When a metallic surface is illuminated with light of wavelength λ\lambda , the stopping potential is XX volt. When the same surface is illuminated by the light of wavelength 2λ2\lambda , stopping potential is X3\dfrac{X}{3}. Threshold wavelength for the metallic surface is:
A) 4λ3\dfrac{{4\lambda }}{3}
B) 4λ4\lambda
C) 6λ6\lambda
D) 8λ3\dfrac{{8\lambda }}{3}

Explanation

Solution

When the light of a certain wavelength strikes on a metal surface, electrons get emitted from the metal surface. This electron is known as photoelectron and the phenomenon of emission of electrons from the metal surface, when exposed to the light, is known as the photoelectric effect. The prefix ‘photo’ is a Greek word that means light.

Complete step by step solution:
We know that Einstein’s photoelectric equation is given by,
eVohc=1λ1λo\dfrac{{e{V_o}}}{{hc}} = \dfrac{1}{\lambda } - \dfrac{1}{{{\lambda _o}}} …….. (1)
Where Vo{V_o} is the stopping voltage, λ\lambda is the corresponding wavelength of the light and λo{{\lambda _o}} is the threshold wavelength of the light.
For a wavelength λ\lambda the corresponding stopping voltage is X. Hence putting, Vo=X{V_o} = X in equation (1) we get,
eXhc=1λ1λo\dfrac{{eX}}{{hc}} = \dfrac{1}{\lambda } - \dfrac{1}{{{\lambda _o}}} ……… (2)
For a wavelength 2λ{2\lambda } the corresponding stopping voltage is X. Hence putting, Vo=X3{V_o} = \dfrac{X}{3} and replace λ{\lambda } with 2λ{2\lambda } in equation (1) we get,
eX3hc=12λ1λo\dfrac{{eX}}{{3hc}} = \dfrac{1}{{2\lambda }} - \dfrac{1}{{{\lambda _o}}} …….. (3)
Dividing equation (2) by equation (3) we get,
3=1λa12λa\Rightarrow 3 = \dfrac{{\dfrac{1}{\lambda } - a}}{\begin{array}{l}\dfrac{1}{{2\lambda }} - a\\\\\end{array}}
Where a=1λoa = \dfrac{1}{{{\lambda _o}}} for the sake of simplification of calculations.
3=1λa12aλ2\Rightarrow 3 = \dfrac{{1 - \lambda a}}{{\dfrac{{1 - 2a\lambda }}{2}}}
36aλ=22aλ\Rightarrow 3 - 6a\lambda = 2 - 2a\lambda
a=14λ\Rightarrow a = \dfrac{1}{{4\lambda }}
1λo=14λ\Rightarrow \dfrac{1}{{{\lambda _o}}} = \dfrac{1}{{4\lambda }}
λo=4λ\therefore {\lambda _o} = 4\lambda

The value of threshold wavelength is found to be 4λ4\lambda hence we can conclude that option B is the correct answer option.

Note: Let us understand the difference between threshold frequency and threshold wavelength.
1. A threshold frequency is the minimum frequency of incident radiation which causes the photoelectric effect to occur. Below the threshold frequency, the photoelectric effect does not occur. The threshold frequency is denoted by νo{\nu _o}. It is measured in Hz.
2. A threshold wavelength is a maximum wavelength of incident radiations which causes the photoelectric effect to occur. Above the threshold wavelength, the photoelectric effect does not occur. The threshold frequency is denoted by λo{\lambda _o}.
The threshold frequency and threshold wavelength have an inverse relationship.