C. Schick et al., SEPARATION OF COMPONENTS OF DIFFERENT MOLECULAR MOBILITY BY CALORIMETRY, DYNAMIC-MECHANICAL AND DIELECTRIC-SPECTROSCOPY, Journal of thermal analysis, 49(1), 1997, pp. 499-511
The relaxation strength at the glass transition for semi-crystalline p
olymers observed by different experimental methods shows significant d
eviations from a simple two-phase model. Introduction of a rigid amorp
hous fraction, which is non-crystalline but does not participate in th
e glass transition, allows a description of the relaxation behavior of
such systems. The question arises when does this amorphous material v
itrify. Our measurements on PET identify no separate glass transition
and no devitrification over a broad temperature range. Measurements on
a low molecular weight compound which partly crystallizes supports th
e idea that vitrification of the rigid amorphous material occurs durin
g formation of crystallites. The reason for vitrification is the immob
ilization of co-operative motions due to the fixation of parts of the
molecules in the crystallites. Local movements (beta-relaxation) are o
nly slightly influenced by the crystallites and occur in the whole non
-crystalline fraction.