A photo-emissive substance is illuminated with a radiation of wavelength λi so that it releases electrons with de-Broglie wavelength λe. The longest wavelength of radiation that can emit photoelectron is λ0. Expression for de-Broglie wavelength is given by :
(m : mass of the electron, h : Planck's constant and c : speed of light)
A
λe=2mc(λih−λ0h)h
B
λe=2mchλ0
C
λe=2mch(λi1−λ01)h
D
λe=2mchλi
Answer
Correct answer:A
Step-by-step solution
Standard Method
Given: Incident radiation has wavelength λi, threshold wavelength is λ0, and the emitted electron has de-Broglie wavelength λe.
Find: The correct expression for λe.
Use Einstein's photoelectric equation and the de-Broglie relation.
The energy of the incident photon is
Eincident=λihc
and the work function is
ϕ=λ0hc
So the maximum kinetic energy of the emitted electron is
Kmax=λihc−λ0hc
Now use
Kmax=2mp2
Therefore,
p=2mKmax=2m(λihc−λ0hc)
The de-Broglie wavelength is
λe=ph
Hence,
λe=2m(λihc−λ0hc)h
which can be written as
λe=2mc(λih−λ0h)h
Therefore, the correct option is A.
Using Momentum Form Directly
Given:Kmax=λihc−ϕ and ϕ=λ0hc.
Find: The expression for electron de-Broglie wavelength.
First substitute the threshold condition into the photoelectric equation:
Kmax=λihc−λ0hc=hc(λi1−λ01)
Now relate kinetic energy and momentum:
Kmax=2mp2
So,
p=2mKmax
Substitute for Kmax:
p=2mch(λi1−λ01)
Then the de-Broglie wavelength becomes
λe=2mch(λi1−λ01)h
This is algebraically the same as option A because
h(λi1−λ01)=λih−λ0h
So option C shows the same derived form, but the solution identifies A as the correct option and option A is the equivalent expression presented in the list.
Therefore, the correct option is A.
Common mistakes
Using ϕ=λ0h instead of ϕ=λ0hc. This is wrong because photon energy is E=λhc. Always include the factor c while converting threshold wavelength to work function.
Writing de-Broglie wavelength as λe=mvh and then stopping without connecting v to kinetic energy correctly. The required link is K=2mp2 or K=21mv2, then substitute into λ=ph.
Missing the subtraction order in λi1−λ01. If the order is reversed, the kinetic energy becomes negative, which is unphysical. The incident photon energy must exceed the work function.
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