Crystallizable polymers often form multiple stacks of uniquely oriented lamellae, which have good registry despite being separated by amorphous fold surfaces. These correlations require multiple synchronized, yet unidentified, nucleation events. Here, we demonstrate that in thin films of isotactic polystyrene, the probability of generating correlated lamellae is controlled by the branched morphology of a single primary lamella. The nucleation density n(s) of secondary lamellae is found to be dependent on the width w of the branches of the primary lamella such that n(s) ∼ w(-2). This relation is independent of molecular weight, crystallization temperature, and film thickness. We propose a nucleation mechanism based on the insertion of polymers into a branched primary lamellar crystal.
In semicrystalline polymers, the segments around the crystallites typically relax significantly slower than in the purely amorphous phase. This results in an, on average, slower dynamics. Here we present a contrary effect in a star-shaped polymer based on a polyhedral oligomeric silesquioxane (POSS) molecule as center and isotactic polystyrene arms. Measurements by means of broadband dielectric spectroscopy reveal a reduction of the mean relaxation time by up to 1 decade. Analyzing the relaxation time distribution unravels three moieties of different dynamics beyond the crystalline fraction. These are assumed to form respective domains: a rigid amorphous fraction around crystallites, a mobile amorphous fraction, and a confined amorphous fraction of enhanced dynamics presumably located around the POSS centers. Probably, the crystallites in combination with the starlike architecture stabilize the average volume which balances the higher density of the growing crystallites by an increase in free volume in the amorphous domains.
Reactor
blend formation of soluble highly isotactic polystyrene (iPS) enables
tailoring of bimodal iPS molar mass distributions containing variable
amounts of ultrahigh molar mass iPS (UHMWiPS). A key feature is the
facile iPS molar mass control, achieved by homogeneous catalytic styrene
polymerization on a MAO-activated titanium bisphenolate catalyst,
using 1,9-decadiene as chain transfer agent. Whereas UHMWiPS (M
w of 947 000 g mol–1) is formed in the absence of the diene, the molar mass M
w increases from 191 000 to 482 000 g mol–1 with decreasing diene/styrene molar ratio. In a cascade
of two parallel reactors, polymerizing styrene in the presence and
the absence of diene, the mixing ratio of the resulting two iPS solutions
governs the UHMWiPS content of the reactor blends (RB-2). Hence, the
contents of iPS and UHMWiPS are varied without affecting the average
molar mass of both blend components. In reactor blends (RB-1), produced
in a single reactor with delayed diene injection, molar mass and polydispersity
of iPS/UHMWiPS as well as molar mass of the iPS fraction and UHMWiPS
depend on the diene/styrene molar ratio and the delay time of the
diene injection. In this study, we investigate the influence of both
iPS molar mass and iPS molar mass distributions on crystallization
behavior and viscoelastic properties. The correlation of zero shear
viscosity with the iPS molar mass exhibits scaling of 3.4, typical
for linear polymer chains. Below 10 wt % UHMWiPS content, bimodal
iPS molar mass distribution enhances processability by shear thinning.
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