H. Marand et al., Influence of structural and topological constraints on the crystallizationand melting behavior of polymers. 2. Poly(arylene ether ether ketone), MACROMOLEC, 33(9), 2000, pp. 3392-3403
The secondary crystallization and its influence on the glass transition are
studied as a function of crystallization temperature and time by different
ial scanning calorimetry for PEEK. The multiple melting behavior resulting
from isothermal annealing from the glass or crystallization from the melt i
s discussed in the context of models considering either a melting-recrystal
lization-remelting process or a bimodal population of primary and secondary
crystals. The heating rate dependence of the multiple melting behavior ind
icates that reorganization of primary crystals occurs during heating for sa
mples annealed from the glassy state but is insignificant for those crystal
lized from the melt. For either mode of crystallization, the high- and low-
temperature endothermic regions are associated with the melting of primary
and secondary crystals, respectively. Investigations of the low endotherm t
ransition temperature and heat of fusion as a function of crystallization t
ime and temperature lead to the following conclusions: the melting temperat
ure of secondary crystals increases linearly with the logarithm of secondar
y crystallization time at a rate, B(T), increasing linearly with decreasing
temperature; the Avrami exponent, which characterizes the initial stage of
secondary crystallization, is constant below ca. 310 degrees C (n = 1/2) b
ut increases gradually with temperature above 310 degrees C; the late stage
of secondary crystallization is characterized by a linear increase in crys
tallinity with logarithm of time. Studies of the evolution of the glass tra
nsition after secondary crystallization indicate that the calorimetric T-g
increases linearly with the logarithm of time at a rate, b(T), increasing w
ith decreasing temperature. Finally, a qualitative model of polymer crystal
lization of semiflexible polymer chains is proposed. This model considers t
he effect of structural constraints (chain stiffness) on the nature of the
amorphous phase after primary crystallization and the effect of topological
constraints (pinning of amorphous chains) on the secondary crystallization
behavior.