Virial decomposition
virial series
The series on the right-hand side of the equation of state of a gas:
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where is the pressure,
is the temperature,
is the specific volume, and
is the Boltzmann constant. The term of the series which contains the
-th virial coefficient
describes the deviation of the gas from ideal behaviour due to the interaction in groups of
molecules.
can be expressed in terms of irreducible repeated integrals
:
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summed over all natural numbers ,
, subject to the condition
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In particular,
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where
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is the volume of the gas, the integration extends over the total volume occupied by the gas, and
is the interaction potential. There is a rule for writing down
for any
in terms of
. The expression obtained after simplification is:
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In practice, only the first few virial coefficients can be calculated.
Power series in , with coefficients expressed in terms of
, can be used to represent equilibrium correlation functions for
particles; a corollary of this fact is that the equation of state can be obtained in a simple manner [3].
There exists a quantum-mechanical analogue of the virial decomposition.
References
[1] | J.E. Mayer, M. Goeppert-Mayer, "Statistical mechanics" , Wiley (1940) |
[2] | R. Feynman, "Statistical mechanics" , M.I.T. (1972) |
[3] | N.N. Bogolyubov, "Problems of a dynamical theory in statistical physics" , North-Holland (1962) (Translated from Russian) |
[4] | G.E. Uhlenbeck, G.V. Ford, "Lectures in statistical mechanics" , Amer. Math. Soc. (1963) |
Virial decomposition. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Virial_decomposition&oldid=16492