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The Maxwell (or Maxwell-Boltzmann) distribution gives the distribution of speeds of molecules in thermal equilibrium as given by statistical mechanics. Defining , where
is the Boltzmann constant,
is the temperature,
is the mass of a molecule, and letting
denote the speed a molecule, the probability and cumulative distributions over the range
are
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(1) |
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(2) |
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(3) |
using the form of Papoulis (1984), where is an incomplete gamma function and
is erf. Spiegel (1992) and von Seggern (1993) each use slightly different definitions of the constant
.
It is implemented in the Wolfram Language as MaxwellDistribution[sigma].
The th raw moment is
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(4) |
giving the first few as
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(5) |
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(6) |
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(7) |
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(8) |
(Papoulis 1984, p. 149).
The mean, variance, skewness, and kurtosis excess are therefore given by
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(9) |
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(10) |
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(11) |
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(12) |
The characteristic function is
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(13) |
where is the erfi function.
REFERENCES:
Papoulis, A. Probability, Random Variables, and Stochastic Processes, 2nd ed. New York: McGraw-Hill, pp. 104 and 148-149, 1984.
Spiegel, M. R. Schaum's Outline of Theory and Problems of Probability and Statistics. New York: McGraw-Hill, p. 119, 1992.
von Seggern, D. CRC Standard Curves and Surfaces. Boca Raton, FL: CRC Press, p. 252, 1993.
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