Derive Planck’s law of black body radiation.
Answer
The probability that a single mode
has energy En = nhν is given by the usual Boltzmann factor
"P(n) =\\frac{exp(-\\frac{h\\nu }{kT}) }{\\sum exp(-\\frac{h\\nu }{kT}) }"
Let x="{exp(-\\frac{h\\nu }{kT}) }=\\frac{h\\nu }{kT}" For classicla limit
So average energy
"U=\\sum E P(n)"
"U=kT"
The energy density of radiation range is
"u(\\nu) d\\nu =\\frac{8\\pi v^2 U d\\nu}{c^3}\\\\ =\\frac{8\\pi hv^3 d\\nu}{c^3(e^(\\frac{h\\nu}{kT}) -1)}"
This is planck radiation distribution law.
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