Derive Stefan-Boltzmann Law from Planck Distribution for blackbody radiation

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SUMMARY

The discussion focuses on deriving the Stefan-Boltzmann law from the Planck distribution for blackbody radiation. The key equation derived is R(T) = (2π^5k^4)T^4 / (15h^3c^2), confirming that total flux is proportional to T^4. Additionally, Wien's displacement law is established, indicating that the maximum value of R(λ,T) occurs at λmT = 2.898 × 10^-3 mK. The discussion also addresses calculations for cosmic background radiation at T = 2.7 K, including peak intensity wavelength, photon energy in eV, and the corresponding electromagnetic spectrum region.

PREREQUISITES
  • Understanding of Planck distribution for blackbody radiation
  • Familiarity with Stefan-Boltzmann law
  • Knowledge of Wien's displacement law
  • Basic calculus for integration and function maximization
NEXT STEPS
  • Learn the derivation of the Stefan-Boltzmann law from the Planck distribution
  • Study the application of Wien's displacement law in astrophysics
  • Explore the implications of blackbody radiation in cosmology
  • Investigate the mathematical techniques for solving integrals involving exponential functions
USEFUL FOR

Students and professionals in physics, particularly those focusing on thermodynamics, astrophysics, and quantum mechanics, will benefit from this discussion.

omegas
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Homework Statement


Starting with the Planck distribution R(\lambda,T) for blackbody radiation.

(a) Derive the blackbody Stefan-Boltzmann law (ie total flux is proportional to T4) by integrating the above expression over all wavelengths. Thus show that
R(T) = (2\pi5k4)T4 / (15h3c2

(b) Show that the maximum value of R(\lambda,T) occurs for \lambdamT = 2.898 * 10-3 mK (this is called Wien's displacement law).

(c) Use Wien's displacement law to determine for the cosmic background radiation with T = 2.7 K
(i) the value of \lambdam for peak intensity
(ii) the energy in eV of photons at this peak intensity, and
(iii) the region of the electromagnetic spectrum corresponding to the peak intesnsity.

Homework Equations



Planck distribution for blackbody radiation:

R(\lambda,T) = (c/4)(8\pi/\lambda4[(hc/\lambda)1/ehc/\lambdakT-1]


The Attempt at a Solution


That was a mouthful. Help please.
 
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here's how to write it in tex (click on it to see how)
R(\lamda,T) <br /> = \frac{c}{4} \frac{8 \pi}{\lambda^4} <br /> (\frac{hc}{\lambda})<br /> (\frac{1}{e^{hc/(\lambda kT)}-1})<br />
ps - check i got it correct

now - how about simplifying and trying the intergal?
 
omegas said:

Homework Statement


Starting with the Planck distribution R(\lambda,T) for blackbody radiation.

(a) Derive the blackbody Stefan-Boltzmann law (ie total flux is proportional to T4) by integrating the above expression over all wavelengths. Thus show that
R(T) = (2\pi5k4)T4 / (15h3c2

(b) Show that the maximum value of R(\lambda,T) occurs for \lambdamT = 2.898 * 10-3 mK (this is called Wien's displacement law).

(c) Use Wien's displacement law to determine for the cosmic background radiation with T = 2.7 K
(i) the value of \lambdam for peak intensity
(ii) the energy in eV of photons at this peak intensity, and
(iii) the region of the electromagnetic spectrum corresponding to the peak intesnsity.

Homework Equations



Planck distribution for blackbody radiation:

R(\lambda,T) = (c/4)(8\pi/\lambda4[(hc/\lambda)1/ehc/\lambdakT-1]

The Attempt at a Solution


That was a mouthful. Help please.

(a) Simplify the expression and integrate it with respect to \lambda over all wavelengths (so the minimum wavelength is 0, what is the maximum wavelength?). You are going to have to make a substitution to get it in a certain form of an integral you can look up.

(b) How do you find the maximum of a function?
 

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