- #1
Nikitin
- 735
- 27
Hi! As my professor is a bit crazy (in a good way), he derived Stefan-Boltzman's law in my intro thermodynamics class. However, since he introduced loads of concepts from statistical mechanics and such I got a bit confused on some points. Anyway:
The first part of the derivation:
My question: Ehm, what happened here? ##df## is a frequency band, ##U## is the total EM energy inside the cavity and ##V## its Volume. Then shouldn't ##N## be the number of photons, and ##<E>## be the mean energy of the photons? Can somebody explain to me how he linked that to "swinging modes" and "density of states" ??
Later he starts talking about frequency space, and density of states and so on. This confuses me. I should probably ask him personally about that once I've got the stuff above cleared up.
The first part of the derivation:
Inside a black body at temperature ##T## you have a cavity, of which inside the energy-density of the EM radiation is ##u## and is proportional to ## T^4##.
Then: ##u(T) = \int d u = \int_0^{\infty} df \cdot \frac{du}{df}##. From there ##\frac{du}{df}= \frac{d(U/V)}{df} = \frac{d( N <E>/V)}{df} =\frac{<E>}{V} \cdot \frac{dN}{df}##, where ##<E>## is the mean energy per state ("swinging mode") and ##dN/df## is the density of states.
My question: Ehm, what happened here? ##df## is a frequency band, ##U## is the total EM energy inside the cavity and ##V## its Volume. Then shouldn't ##N## be the number of photons, and ##<E>## be the mean energy of the photons? Can somebody explain to me how he linked that to "swinging modes" and "density of states" ??
Later he starts talking about frequency space, and density of states and so on. This confuses me. I should probably ask him personally about that once I've got the stuff above cleared up.
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