QM- Stefan's constant vs radiation constant

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SUMMARY

The discussion centers on the relationship between Stefan's constant and the radiation constant in the context of Planck's formula for energy density. The total energy density is proven to be ρ(T) = aT^4, where a = 8π^5k^4/(15h^3c^3). The participant expresses confusion regarding the connection to the Stefan-Boltzmann law, specifically the derivation of P = σT^4 and the distinction between the radiation constant (a = 4σ/c) and Stefan's constant. The inquiry seeks clarity on the differences in derivation and utility between these constants.

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QM-- Stefan's constant vs radiation constant

Homework Statement



(a) Using Planck's formula for the energy density ρ(λ,T), prove that the total energy density is given by ρ(T)=aT4 where a = 8π5k4/(15h3c3). (b) Does this agree with the Stefan-Boltzmann law for the total emissive power?

The Attempt at a Solution



I had no problem with the proof in part (a), starting with the equation
ρ(T)dλ = 8πhc/λ5 * dλ/(ehc/λkT-1) and integrating over λ 0→∞.

However, I am confused by the question in part (b). The answers are obviously related. I know that a, the radiation constant, is equal to 4σ/c, and I know you can derive the precise Stefan-Boltzmann equation from Planck's formula. I also suspect the professor is looking for an answer other than "no" or "sort-of." Does anyone know where the difference between that derivation and the one I completed and the one that yields P = σT4 is? What is the utility difference between the radiation constant and Stefan's constant?

Thanks guys!
 
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Hmm... have a look at the Wikipedia article on Planck's law and see if it suggests anything :wink:
 

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