Energy Density of Blackbody Radiation

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SUMMARY

The discussion focuses on deriving the expression for the total energy density of blackbody radiation for frequencies less than a specified frequency, ν₀, under the condition that hν₀ << kT. The derived formula is p(<ν₀) = (8πkT/3c³)ν₀³, which is obtained by integrating Planck's Law within the limits from 0 to ν₀. The Rayleigh-Jeans formula is also referenced, indicating the relationship between energy density and temperature. The solution is confirmed to be correct by participants in the discussion.

PREREQUISITES
  • Understanding of Planck's Law for blackbody radiation
  • Familiarity with the Rayleigh-Jeans formula
  • Knowledge of thermodynamic concepts such as temperature (T) and Boltzmann's constant (k)
  • Basic calculus skills for performing integration
NEXT STEPS
  • Study the derivation of Planck's Law in detail
  • Explore applications of the Rayleigh-Jeans formula in physics
  • Learn about the implications of blackbody radiation in astrophysics
  • Investigate the relationship between energy density and temperature in thermodynamics
USEFUL FOR

Students and professionals in physics, particularly those focusing on thermodynamics, quantum mechanics, and astrophysics, will benefit from this discussion.

stefan10
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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!
 
Last edited:
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Looks good to me.
 

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