Cluster integrals

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In an ideal gas there are no intermolecular interactions. However, in an imperfect or real gas, this is not so, and the second virial coefficient is other than zero. Mayer and Mayer developed a theoretical treatment of the virial coefficients in terms of cluster integrals.

The simplest cluster is that consisting of a single molecule, not bound to any other. A cluster of three specified identical molecules, i, j and k may be formed in any of four ways:


The first three cluster integrals are (Eq. 13.6 in [1])

b1=11!V∫dτ1=1

Ref. 1 Eq. 13.7:

b2=12!V∬f(r12)dτ2dτ1=12∫0∞4πr2f(r)dr

and Ref. 1 Eq. 13.8:

b3=13!V∭(f31f21+f32f31+f32f21+f32f31f21)dτ3dτ2dτ1

using the Mayer f-function notation.

Irreducible clusters[edit]

Irreducible clusters are denoted by βk

β1=∫f31dτ3=1V∬f12dτ1dτ2=∫0∞4πr2f(r)dr

note b2=12β1.


β2=12V∭f32f31f21dτ1dτ2dτ3

note b3=12β12+13β2

β3=16V⨌(3f43f32f21f41+6f43f32f21f41f31+f43f32f21f41f31f42)dτ1dτ2dτ3dτ4

note b4=23β13+β1β2+14β3

Hellmann and Bich diagrams[edit]

Hellmann and Bich have rederived the virial equation of state from the grand canonical partition function without restricting themselves to pairwise intermolecular pair potentials [2]. This leads to expressions for the virial coefficients that, for B6 and beyond, require the evaluation of far fewer diagrams when compared to the original diagrams of Mayer or to the reformulation of Ree and Hoover [3].

See also[edit]

References[edit]

Related reading