Crystallization behaviors of crystallizable poly(ethylene terephthalate co
ethylene isophthalate) with different molar ratios of polyethylene terephth
alate (PET) to polyethylene isophthalate: (PEI) were studied both non-isoth
ermally and isothermally by differential scanning calorimetry (DSC). Avrami
and Ozawa plots were used to describe the non-isothermal crystallizations.
However, the Avrami treatment cannot predict the mechanisms of non-isother
mal crystallizations for the above copolyesters, while the Ozawa explanatio
n can be taken to reveal that the non-isothermal crystallization is dominat
ed by heterogeneous nucleation. The activation energies of crystallization
were calculated from the Kissinger equation. The copolyester 90/10 shows sy
nergistic effects on non-isothermal crystallization, in that it has the low
est activation energy of crystallization. Isothermal crystallizations were
explained by Avrami plots. From lower degrees of supercooling to higher one
s, the crystals of the copolyesters grow from low dimension to multidimensi
ons, but the crystallization rates become lower. The percentage of spheruli
te growth of the copolyester 100/0 (PET homopolymer) is higher than that of
the other copolyesters under the same degree of supercooling. Equilibrium
crystallization temperatures (T-c(0)) and melting temperatures (T-m(0)) wer
e postulated respectively. T-c(0) and T-m(0) decrease with the increasing c
omposition of PEI, indicating that the equilibrium crystals of the copolyes
ters become imperfect. With involvement of PEI, the copolyester is not like
ly crystallizable perfectly and the crystal becomes less perfect. (C) 1999
Elsevier Science Ltd. All rights reserved.