Plank's law state that the spectral radiance "{{B}_{\\nu }}" of a physical body for frequency "\\nu" at absolute temperature T is given by
where k is the Boltzmann constant, h is the Planck constant, and c is the speed of light in the medium. Spectral radiance "{{B}_{\\nu }}" is the power, emitted per unit area of the body, per unit solid angle of emission, per unit frequency.
Considering that
"\\nu =\\frac{c}{\\lambda }"where λ is the radiation wavelength, the spectral radiance can also be expressed per unit wavelength λ instead of per unit frequency, that is
"{{B}_{\\lambda }}\\left( \\lambda ,T \\right)=\\frac{2h{{c}^{2}}}{{{\\lambda }^{5}}}\\frac{1}{{{e}^{\\frac{hc}{\\lambda kT}}}-1}"
There is a relationship between these two forms of Plank's law
where "d\\nu =-\\frac{c}{{{\\lambda }^{2}}}d\\lambda" holds true.
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