Solid-State NMR Characterization of the Chemical Defects
and Physical Disorders in α Form of Isotactic Poly(propylene)
Synthesized by Ziegler–Natta Catalysts
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Abstract
The
order–disorder phenomenon and spatial heterogeneity
of chain packing, partitions of stereodefects, and molecular dynamics
of α form of isotactic polypropylene (<i>i</i>PP)
samples, which are synthesized by Zieglar–Natta catalysts,
are investigated by solid-state (SS) NMR. High-resolution <sup>13</sup>C NMR under high-power TPPM decoupling at field strengths of 110
kHz allows observation of the order–disorder phenomenon in
the chain-packing structures of α form. High isotacticity samples
(isotacticity at pentad level, ⟨<i>mmmm</i>⟩
= 99.4%) give a maximum ordered packing (α<sub>2</sub>) fraction
of 66% at crystallization temperature (<i>T</i><sub>c</sub>) of 155 °C while low stereoregularity samples (⟨<i>mmmm</i>⟩ = 91.0%) have only 47% at the same <i>T</i><sub>c</sub>. However, <i>M</i><sub>w</sub> (58.7–982
kg/mol) does not play a significant role in ordered packing formation.
Using <sup>13</sup>C-labeled CH<sub>3</sub> of <i>i</i>PP,
direct spatial correlations between the α<sub>2</sub> and α<sub>1</sub> structures are investigated by <sup>13</sup>C detection of
two-dimensional (2D) <sup>1</sup>H–<sup>1</sup>H spin-diffusion
(CHHC) experiments. The time dependence of the spin-diffusion polarization
transferred signal intensities determines the average domain size
of the α<sub>1</sub> and α<sub>2</sub> structures of <i>i</i>PP crystallized at 150 °C, which was found to be 40
nm under an assumption of 2D spin diffusion. Additionally, the <sup>13</sup>C filter CPMAS NMR spectrum on <sup>13</sup>C CH<sub>3</sub>-labeled <i>i</i>PP demonstrates that chemical defect is
almost excluded from the crystalline region at <i>T</i><sub>c</sub> = 150 °C (defect free crystal) while ca. 2% is in melt
quench sample. Moreover, <sup>13</sup>C centerband-only detection
of exchange experiments on α<sub>2</sub>-rich sample with highest
⟨<i>mmmm</i>⟩ = 99.4% indicate that crystalline
dynamics follows a single Arrhenius plot with an activation energy
of 116 kJ/mol across reported order–disorder transition temperatures
(157–159 °C)