  A model for the radial distribution function $g(r)$ of a square-well fluid of
variable width previously proposed [S. B. Yuste and A. Santos, J. Chem. Phys.
{\bf 101}, 2355 (1994)] is revisited and simplified. The model provides an
explicit expression for the Laplace transform of $rg(r)$, the coefficients
being given as explicit functions of the density, the temperature, and the
interaction range. In the limits corresponding to hard spheres and sticky hard
spheres the model reduces to the analytical solutions of the Percus-Yevick
equation for those potentials. The results can be useful to describe in a fully
analytical way the structural and thermodynamic behavior of colloidal
suspensions modeled as hard-core particles with a short-range attraction.
Comparison with computer simulation data shows a general good agreement, even
for relatively wide wells.
