The triangle distribution function f((3)) for three mutual near neighbors i
n the plane describes basic aspects of short-range order and statistical th
ermodynamics in two-dimensional many-particle systems. This paper examines
prospects for constructing a self-consistent calculation for the rigid-disk
-system f((3)). Wr present several identities obeyed by f((3)). A rudimenta
ry closure suggested by scaled-particle theory is introduced. In conjunctio
n with three of the basic identities, this closure leads to an unique f((3)
) over the entire density range, The pressure equation of state exhibits qu
alitatively correct behaviors in both the low-density and the close-packed
limits, but no intervening phase transition appears. We discuss extensions
to improved disk closures. and to the three-dimensional rigid-sphere system
.