  By means of a Quadratic Diffusion Monte Carlo method we have performed a
comparative analysis between the Aziz potential and a revised version of it.
The results demonstrate that the new potential produces a better description of
the equation of state for liquid $^4$He. In spite of the improvement in the
description of derivative magnitudes of the energy, as the pressure or the
compressibility, the energy per particle which comes from this new potential is
lower than the experimental one. The inclusion of three-body interactions,
which give a repulsive contribution to the potential energy, makes it feasible
that the calculated energy comes close to the experimental result.
