The Ising model has been an important theoretical tool in the understanding
of phase transitions in ferroelectric materials. We first review how it re
lates to the underlying physics of order-disorder phase transitions in thes
e systems, as well as mean-field results for the spontaneous polarization a
nd the dielectric constant near the critical temperature. For hydrogen-bond
ed ferroelectrics, a term of interaction with an external transverse field
is necessary to account for proton tunneling between the two minima of a. d
ouble-well potential. Finally, me discuss both experimental and theoretical
results for the problems of proton-lattice interactions, central peak dyna
mics, dynamical behavior of pseudo-one-dimensional ferroelectrics and press
ure effects on hydrogen bonded ferroelectrics.