The strengths and short-comings of the point-dipole model for polar fluids of
spherical molecules are illustrated by considering the physically more relevant
case of extended dipoles formed by two opposite charges ±q separated by a
distance d (dipole moment μ=qd). Extensive Molecular Dynamics
simulations on a high density dipolar fluid are used to analyse the dependence
of the pair structure, dielectric constant \eps and dynamics as a function of
the ratio d/σ (\sig is the molecular diameter), for a fixed dipole
moment μ. The point dipole model is found to agree well with the extended
dipole model up to d/\sig \simeq 0.3. Beyond that ratio, \eps shows a
non-trivial variation with d/\sig. When d/\sig>0.6, a transition is
observed towards a hexagonal columnar phase; the corresponding value of the
dipole moment, \mu^2/\sig^3 k T=3, is found to be substantially lower than
the value of the point dipole required to drive a similar transition.Comment: 10 pages, 11 figures; Paper submitted to Molecular Physic