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Born and Green's Theory of Imperfect Gases

Abstract

As is well known, the Born and Green theory of classical fluids1 makes use of the so-called ‘super-position-principle’ first employed, in this connexion, by Kirkwood and Boggs2. Using this hypothesis, a non-linear integral equation is obtained for the radial distribution function, from which other properties of the fluid, such as its pressure, can be calculated.

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References

  1. Born, M., and Green, H. S., “A General Kinetic Theory of Liquids”, chapters 1 and 2 (Cambridge, 1949).

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  2. Kirkwood, J. G., and Boggs, E. M., J. Chem. Phys., 10, 394 (1942).

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  3. Mayer, J. E., et al., J. Chem. Phys., 5, 67, 74; 6, 87, 101 (1937).

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  4. Rodriguez, A. E., Proc. Roy. Soc., A, 196, 73 (1949).

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  5. Fowler, R. H., and Guggenheim, A. E., “Statistical Thermodynamics”, 289 (Cambridge, 1939).

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RUSHBROOKE, G., SCOINS, H. Born and Green's Theory of Imperfect Gases. Nature 167, 366–367 (1951). https://doi.org/10.1038/167366a0

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