The kinetic fragility of a glass-forming
liquid is an important
parameter to describe its molecular mobility. In most polymers, the
kinetic fragility index obtained from the glassy state by thermally
stimulated depolarization current is lower than the one determined
in the liquid-like state by dielectric relaxation spectroscopy, as
shown in this work for neat polylactide (PLA). When PLA is plasticized
to different extents, the fragility calculated in the liquid-like
state progressively decreases, until approaching the value of fragility
calculated from the glass, which on the other hand remains constant
with plasticization. Using the cooperative rearranging region (CRR)
concept, it is shown that the decrease of the fragility in the liquid-like
state is concomitant with a decrease of the cooperativity length.
By splitting the fragility calculated in the liquid, in two contributions:
volume and energetic, respectively, dependent and independent on cooperativity,
we observed that the slope of the fragility plot in the glass is equivalent
to the energetic contribution of the fragility in the liquid. It is
then deduced that the difference between the slopes of the relaxation
time dependence calculated in both glass and liquid is an indicator
of the cooperative character of the segmental relaxation when transiting
from liquid to glass. As the main structural consequence of plasticization
lies in the decrease of interchain weak bonds, it is assumed that
these bonds drive the size of the CRR. In contrast, the dynamics in
the glass are independent on plasticization structural effects.