Under isothermal crystallization
(T
c) from the melt, polyacetals spaced
by 12, 18, 19, or 23 methylenes
develop two or three distinctive layered polymorphs. The polymorphs
formed in the lowest T
c range are kinetically
favored (hexagonal and Form I) and characterized by highly nucleated
small axialites up to T
c very close to
their melting point. In the higher range of T
c, a thermodynamically more stable Form II develops that melts
at 5–8 degrees higher temperatures and forms large spherulites.
Form I and Form II overlap in a very small range of T
c. While the overall crystallization kinetics of Form
I display the usual negative temperature coefficient, an inversion
of the dependence of the rate of Form II with temperature occurs when
approaching from above the narrow T
c range
where Form I and Form II coexist. The inversion is attributed to a
competition in nucleation between Form I and Form II. Just before
inception of Form II, the crystallization rate is so low that it becomes
basically extinguished. The degree of crystallinity recovers when
pure Form II develops with a small increase in T
c. Although in the overlapping range, the growth rates of Form
I are significantly lower than those of Form II, compared at a fixed
undercooling, the rates of Form I are one order of magnitude higher
than those of Form II. The difference is attributed to a two to six
times higher energy barrier for nucleation of Form II, calculated
from analysis of growth rate data according to surface nucleation
theory. Such a difference explains the observed variation in nucleation
density between the two polymorphs. A minimum in the growth rate of
Form I of PA-12, consistent with the effect of “self-poisoning”,
occurs at T
c approaching the melting point
of the hexagonal phase from above.