Planck's's radiation function is the function
|
(1)
|
which is normalized so that
|
(2)
|
However, the function is sometimes also defined without the numerical normalization factor of
(e.g., Abramowitz and Stegun 1972, p. 999).
The first and second raw moments are
where
is Apéry's constant, but higher order raw
moments do not exist since the corresponding integrals do not converge.
It has a maximum at (OEIS A133838),
where
|
(5)
|
and inflection points at (OEIS A133839)
and
(OEIS A133840), where
|
(6)
|
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References
Abramowitz, M. and Stegun, I. A. (Eds.). "Planck's Radiation Function." §27.2 in Handbook
of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, 9th printing.
New York: Dover, p. 999, 1972.Sloane, N. J. A. Sequences
A133838, A133839,
A133840 in "The On-Line Encyclopedia of
Integer Sequences."Referenced on Wolfram|Alpha
Planck's Radiation Function
Cite this as:
Weisstein, Eric W. "Planck's Radiation Function."
From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/PlancksRadiationFunction.html
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