Deriving the rayleigh-jeans limit of planck law of radiation

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SUMMARY

The discussion focuses on deriving the Rayleigh-Jeans limit from Planck's law of radiation. The original formula for Planck's law is given as \( B(\nu) = \frac{2\,h\,\nu^3}{c^2(e^{h\nu/kT}-1)} \). The user, Marius, initially attempts to apply L'Hôpital's rule to show that as frequency approaches zero, the limit yields the Rayleigh-Jeans law \( B(\nu) = \frac{2\nu^2kT}{c^2} \). After realizing an error in his calculations, he corrects it by using the approximation \( e^{h\nu/kT} \approx 1 + h\nu/kT \) to derive the correct limit.

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Jonsson
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Hello there,

Plack law of radiation
$$
B(\nu) = \frac{2\,h\,\nu^3}{c^2(e^{h\nu/kT}-1)}
$$

I want to show that for small frequencies, Reyleigh-Jeans law:
$$
B(\nu) = \frac{2\nu^2kT}{c^2}
$$
is correct.

I take the limit of Planck law as ##\nu \to 0## using l'hopital rule:
$$
\lim_{\nu \to 0} \frac{2\,h}{c^2} \frac{\nu^3}{e^{h\nu/kT}-1} \stackrel{\text{l'H}}{=} \lim_{\nu \to 0} \frac{2\,h}{c^2} \frac{3\nu^2kT}{e^{h\nu/kT}h} = 0
$$

I am off by a factor of 3. What is wrong with my maths?

Thank you for your time.

Kind regards,
Marius
 
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Oh, I got it worked out. I just write, ##e^{h\nu/kT} \approx 1 + h\nu/kT##, and substitute this into Planck law of radiation.
 

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