Abstract
The theory of fluids based on the radial distribution function,
g(r)
, is related to the direct correlation function,
f(r)
, of scattering theory. The simplest form of the Born-Green theory is shown to be intimately related to the first approximation to
f(r)
. The second approximation to
f(r)
is considered in detail, and shown to effect a considerable improvement on earlier theories. It leads to a critical point at which
p/ρkT
=⅓. Fournet’s application of the Born-Green theory to X-ray scattering by fluids is shown to be correct only to the first power in the density ρ. The terms in ρ and ρ
2
are considered in detail for the case of hard spheres.
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