A detailed discussion is given of the predictions of the Landau-Devonshire
theory for the behavior of thin ferroelectric films. It is assumed that the
phase transition in the bulk is second order, and the theory is extended b
y the inclusion in the free-energy density of a term proportional to \delP\
(2) together with a boundary condition involving an extrapolation length de
lta. Expressions for the polarization profile P(z) are given in terms of Ja
cobi elliptic functions; some of these are in a clearer and simpler form th
an has been available previously. Interesting analytic results for the entr
opy in terms of elliptic integrals and elliptic functions are also presente
d. Graphical illustrations of the main results are included. Careful consid
eration is given to the nature of the phase transition, and it is concluded
that it is second order in all cases.