We have studied melting of poly(butylene
succinate), isothermally
crystallized over a wide temperature range, employing a combination
of the Hoffman–Weeks plot and the Gibbs–Thomson crystallization
line, determined by small-angle X-ray scattering measurements. A change
in the slope
α
of the Hoffman–Weeks
(H–W) line, accompanied by a change of the slope of the crystallization
line, was observed for crystallization temperatures higher than 110
°C.
α
was reaching a value
of 1, implying that no intersection point between the H–W line
and the T
m
= T
c
line could be obtained. (T
m
is the measured melting temperature
and T
c
is the temperature
at which the sample was crystallized). This observation was corroborated
by the crystallization line, which was found to be parallel to the
melting line for T
c
>
110 °C. We relate these changes in slope to different stabilization
mechanisms of the secondary nuclei at the growth front of polymer
lamellar crystals. For T
c
> 110 °C, secondary nuclei are proposed to be stabilized
by
coalescence of neighboring nuclei, all having a small width. By contrast,
for T
c
> 110 °C,
the number density of secondary nuclei is low and thus their coalescence
is rare. Accordingly, nuclei are stabilized by growing in size, mainly
increasing their width.