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I checked one of the other questions on this - and I still seem to have a different equation than they offer (as far as I can tell). I'll use the notation the books used, btw.

In one of my reference books, they first derived the Rayleigh-Jeans formula (I can include how they derived it, if that will help):

$$u(v,T) = \frac{8\pi v^2}{c^3}k_BT,$$

($k_B$ - Boltzmann constant, $v$ - frequency, $T$ - temperature)

Then they "re-derived" Planck's formula by replacing the integral with the summation and ended up with:

$$u(v,T) = \frac{8\pi v^2}{c^3} \frac{hv}{e^{\frac{hv}{kT}}-1}$$

($h$ - Planck constant)

However, the next book I looked at puts Planck's Law in terms of $\lambda$:

$$u(\lambda) = \frac{8 \pi hc\lambda^{-5}}{e^{\frac{hc}{\lambda kT}}-1} = \frac{8\pi}{\lambda^5}\frac{hc}{e^{\frac{hc}{\lambda kT}}-1}$$

By the way, the Rayleigh-Jeans law the second book derived is:

$$u(\lambda) = \frac{8\pi kT}{\lambda^{-4}}$$

My questions are:

If both functions are valid, why are only one of them mentioned in each book? Why can't I find the function with $v^2$ on Wiki, or PSE... is the first book wrong?

galois
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Both expressions are equivalent; they are simply calculating slightly different quantities. The first one gives the energy density per unit frequency, and the second one gives the energy density per unit wavelength. These two differ by a square of the frequency / wavelength because one unit of frequency represents a larger range of wavelengths at low frequency than at high frequency. If you do the change of variables correctly you can go back and forth between the two.

Emilio Pisanty
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