  A chiral pion-nucleon amplitude supplemented by the HJS subthreshold
coefficients is used to calculate the the long range part of the two-pion
exchange nucleon-nucleon potential. In our expressions the HJS coefficients
factor out, allowing a clear identification of the origin of the various
contributions. A discussion of the configuration space behaviour of the loop
integrals that determine the potential is presented, with emphasis on
cancellations associated with chiral symmetry. The profile function for the
scalar-isoscalar component of the potential is produced and shown to disagree
with those of several semi-phenomenological potentials.
