Energy Density of Blackbody Radiation

AI Thread Summary
The discussion focuses on deriving the total energy density of blackbody radiation for frequencies less than a specified threshold, ν₀, under the condition that hν₀ is much less than kT. The integration of Planck's Law is performed, leading to the simplification of the energy density expression. The Rayleigh-Jeans formula is applied to obtain the energy density as a function of temperature and frequency. The final result for the total energy density below ν₀ is presented as p(<ν₀) = (8πkT/3c³)ν₀³. The solution appears to be correct based on the calculations provided.
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Homework Statement



\mbox{Let} \ p(&lt; \nu_{0}) \mbox{be the total energy density of blackbody radiation in all frequencies less than} \ \nu_{0}, \mbox{where} \ h \nu_{0} &lt;&lt; kT. \mbox{Derive an expression for} \ p (&lt; \nu_{0})

Homework Equations



p(v) dv = \dfrac{8 \pi h} {c^3} \dfrac {\nu^3}{e^\frac{h\nu}{kT} -1} dv

The Attempt at a Solution



We want to find the total energy density, so that means we'll have to integrate the Planck's Law. The limits of integration will be from 0 to v-knot.

h \nu &lt; h \nu_{0} &lt;&lt; KT \Rightarrow h \nu &lt;&lt; KT

Which if we simplify for this limit gives:

p(v) dv = \dfrac{8 \pi h} {c^3} \dfrac {\nu^3}{e^\frac{h\nu}{kT} -1} dv

p(v) dv = \dfrac{8 \pi h} {c^3} \dfrac {\nu^3}{\dfrac{h\nu}{kT} +1 -1} dv

p(v) dv = \dfrac{8 \pi h} {c^3} \dfrac {\nu^3}{\frac{h\nu}{kT} } dv

p(v) dv = \dfrac{8 \pi KT}{c^3} \nu^2 dv \ \mbox{Rayleigh-Jeans Formula}

p(&lt;v_{0}) = \dfrac{8 \pi KT}{c^3}\int _ {0} ^{\nu_{0}} \nu^2 dv

p(&lt;v_{0}) = \dfrac{8 \pi KT}{3 c^3}\nu_{0}^3

Is there anything wrong? Thank you very much!
 
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Looks good to me.
 
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