文摘
The chain packing, crystal thickness, molecular dynamics, and melting temperature of 伪-form isotactic polypropylene (iPP) drawn uniaxially at high temperatures of 100鈥?50 掳C were investigated using solid-state (SS) NMR and DSC. Two types of iPP samples with disordered (伪1) and relatively ordered (伪2-rich) packing structures were prepared via different thermal treatments and drawn up to an engineering strain (e) of approximately 20. High-resolution 13C NMR detected continuous 伪2 鈫?伪1 transformations in the original 伪2-rich samples over the entire deformation range at all drawing temperatures (Tds). A sudden 伪1 鈫?伪2 transformation was found to occur in the original 伪1 sample in the small e range of approximately 3鈥? at Td = 140 掳C. Then, in the late stage, the newly grown 伪2 structure reversely transformed into 伪1 structure with further increase in e, as observed in the original 伪2-rich sample. These results indicate that at least two different processes are involved in large deformations. On the basis of crystallographic constraints, the continuous 伪2 鈫?伪1 transformation over the entire deformation range is attributed to molecular-level melting and recrystallization facilitated by chain diffusion. The steep 伪1 鈫?伪2 transformation in the smaller e range is assigned to isotropic melting and recrystallization induced by stress. After the large deformations (e 鈮?20) of the original 伪2-rich and 伪1 samples at Td = 150 and 140 掳C, respectively, 1H spin diffusion verified increases in the crystal thickness in both the former (14.1 at e = 0 鈫?20.1 nm at e = 20) and the latter (9.2 鈫?17.0 nm). Centerband-only detection of exchange (CODEX) NMR at 120 掳C demonstrated that the correlation time (蟿c) of the helical jump for the former drastically decreased from 蟿c = 52.4 卤 5.2 at e = 0 to 9.3 卤 1.8 ms at e = 20 but slightly increased from 4.2 卤 1.3 to 7.1 卤 0.9 ms for the latter. Additionally, DSC indicated that the melting temperature (Tm) for the former decreased considerably from 173 掳C at e = 0 to 165 掳C at e = 20, whereas the melting temperature (Tm) remained nearly invariant at 163 掳C for the latter. On the basis of these findings, we conclude that the local packing structure plays a crucial role in determining the molecular dynamics of the stems and Tm of largely deformed iPP materials. The established relations among the structures, the dynamics, and the thermal properties provide a useful guide to achieving improved properties of iPP materials under processing.