How do I find the work function of a metal using black body radiation?

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SUMMARY

The discussion focuses on calculating the work function of a metal using black body radiation principles. The initial peak emission occurs at a wavelength of 9000 Angstroms, and upon increasing the temperature, the total radiation emitted increases by a factor of 81. The correct approach involves applying Wein’s displacement law and Stefan’s law, leading to a final temperature of 9660 Kelvin and an energy of incident radiation calculated as 6.63 x 10-19 Joules. The discrepancy in answers arises from assumptions made regarding the uniformity of flux and the nature of the black body.

PREREQUISITES
  • Understanding of Wein’s displacement law
  • Familiarity with Stefan-Boltzmann law
  • Knowledge of photoemission and work function concepts
  • Basic principles of quantum mechanics, specifically energy quantization (E=hv)
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  • Study the derivation and applications of Wein’s displacement law
  • Explore Stefan-Boltzmann law in detail, including its implications for black body radiation
  • Learn about photoemission and its relationship with work function in metals
  • Investigate the quantum mechanics of energy levels in hydrogen and other atoms
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Students in physics, particularly those studying thermodynamics and quantum mechanics, as well as researchers and educators involved in materials science and photonics.

Amith2006
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Homework Statement


1)The peak emission from a black body at a certain temperature occurs at a wavelength of 9000 Angstrom. On increasing its temperature the total radiation emitted is increased 81 times. At the initial temperature, when the peak radiation from the black body is incident on a metal surface, it does not cause any photoemission from the surface. After the increase of temperature, the peak radiation from the black body causes photoemission. To bring these photo electrons to rest, a potential equivalent to the excitation energy between n=2 and n=3 Bohr levels of Hydrogen atom is required. Find the work function of the metal.


Homework Equations


According to Wein’s displacement law,
[lambda1(max.) x T1] = 2.898 x 10^(-3) metre-Kelvin

According to Stefan’s law,
Energy of incident radiation(E2) = (sigma) x T^4


The Attempt at a Solution



I have doubt only in the first part of the problem. So I haven’t worked out the entire problem.
I solved it in the following way:

Let T1 and T2 be the initial and final temperatures respectively. Let lambda1(max.) and lambda2(max.) be the initial and final wavelengths respectively. Let E1 and E2 be the initial and final energy of the radiations respectively.
According to Stefan’s law,
E is proportional to T^4
Hence,
E1/E2 = [T1/T2]^4
Therefore,
T2 = 3T1 {since given that E2/E1 = 81}
According to Wein’s displacement law,
[lambda1(max.) x T1] = 2.898 x 10^(-3) metre-Kelvin
Hence, T1 = 3220 Kelvin
Hence, T2 = 3T1 = 9660 Kelvin
According to Stefan’s law,
Energy of incident radiation(E2) = (sigma) x T^4
= 5.67 x 10^(-8) x (9660 x 10^(-10))^4
= 4.94 x 10^(-32) Joules


The solution given in my book is as follows:

According to Stefan’s law,
E is proportional to T^4
Hence,
E1/E2 = [T1/T2]^4
Therefore,
T2 = 3T1 {since given that E2/E1 = 81}
According to Wein’s displacement law,
[lambda(max.) x T] = constant
i.e. [lambda1(max.) x T1] = [lambda2(max.) x T2]
lambda2(max.) = 3000 Angstrom
Energy of incident radiation(E2) = hc/ lambda2(max.) = 6.63 x 10^(-19) Joules

Why do I get 2 different answers?
 
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You assumed a lot of things when you use Stefan's Law: that it was a perfect blackbody, and the flux was uniform.

The solution your book gave is correct because it does everything through Wein's Law, and then uses the fact that E=hv=hc/lambda.
 
Thats cool! Thanks.
 

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