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Question

In a photoelectric effect set-up a point source of light of power 3.2×103 W emits monoenergetic photons of energy 5.0 eV. The source is located at a distance of 0.8 m from the centre of a stationary metallic sphere of work function 3.0 eV and of radius 8.0×103m. The efficiency of photoelectron emission is one-for every 106 incident photons. Assume that the sphere is isolated and initially natural and that photoelectron are instantly swept away after emission.
Calculator the number of photoelectron emitted per second.
Find the ratio of the wavelength of incident light to the de-Broglie wavelength of the fastest photoelectron emitted.
It is observed that the photoelectron emission stop at a certain time t after the light source is switch on. Why?
Evaluate the time t.

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Solution

Energy of emitted photons
E1=0.5 eV=8×1019
Energy emitted per second by the source
E2=3.2×103 J
No. of photons emitted per second =E2E1=4×1015
No. of photons incident on the sphere per second
n=4×10154π(0.8)2×π(8×103)21011 per second
No, of photoelectron emitted per second
n=1011106=105 per second
Max. K.E. of photo electron
kmax= Energy of incident photons work function =2 eV=3.2×1019 J
de-Broglie wavelength of these photoelectrons
λ1=h2kmaxme=8.68 A
wavelength of incident light
λ2=123755=2475 A
The desired ratio is λ1/λ2
Emission of photoelectrons is stopped when its potential is equal to the stopping potential required of the fastest moving electrons
kmax=2eV
Stopping potential v0=2 volt
2=kq/r
q=1.78×1012C
t=q105×1.6×1019
t111 seconds.
1038557_1013847_ans_a97530c063304e7691ed940b8dc321bc.png

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