The geometric Gibbs equation describes how the available space and correspo
nding surface area of a single- component hard particle fluid varies with t
he system density. When a closure condition is introduced, i.e., an additio
nal equation describing how the surface area depends on the available space
, the geometric Gibbs equation reduces to a second-order differential equat
ion indicating how the available space varies with the system density. Solu
tion of this new equation provides another route to the determination of th
e chemical potential and pressure of the hard particle fluid. The simplest
proposed closure condition yields the properties of fully penetrable sphere
s. A modified closure condition is suggested, and its connection to thermop
hysical properties is derived. An extension of the exact form of the closur
e condition for the one-dimensional hard rod fluid yields a reasonably good
approximation of the properties of the hard sphere fluid at low density, a
nd is found to be the required form for densities above the freezing densit
y. The simple form of the closure condition and its connection to bulk prop
erties may be used to help suggest future closure relations.