TY - JOUR
T1 - Thermal Stability of Shear-Induced Crystal Nuclei of Poly(l -lactic acid)
AU - Du, Mengxue
AU - Jariyavidyanont, Katalee
AU - Zhang, Rui
AU - Rhoades, Alicyn M.
AU - Schick, Christoph
AU - Androsch, René
N1 - Funding Information:
MD and RA gratefully acknowledge financial support by the Deutsche Forschungsgemeinschaft (DFG) (grant number AN 212/20). Further funding was provided by the European Social Funds (ESF) and the Federal State Saxony-Anhalt in Germany, within the International Graduate School AgriPoly at the Martin Luther University Halle-Wittenberg.
Publisher Copyright:
© 2022 American Chemical Society.
PY - 2022/10/14
Y1 - 2022/10/14
N2 - Knowledge of the conditions required to obtain an isotropic melt of the polymer of interest, which before was subjected to shear and crystallization, is important for understanding and prediction of crystallization in polymer processing. In this work, the thermal stability of crystallization precursors of qualitatively different structures, namely, classical crystal remnants and oriented shish-like nuclei, is analyzed for poly(l-lactic acid) (PLLA). Shearing the melt at different rates leads to generation of shish-like and point-like nuclei which grow at identical temperature to crystals of similar stability/melting temperature. Analysis of the crystallization kinetics and of the semicrystalline morphology by differential scanning calorimetry and polarized-light optical microscopy, respectively, after subjecting the melt to different maximum temperatures, showed that disordering/isotropization of remnants of crystals, which melt close to 179 °C, occurs in a temperature window about 5-10 K higher than the melting temperature. Shish-like nuclei, generated at 135 °C during shearing the melt 10 s at 2 s-1, survive heating to a higher temperature than in the case of self-nuclei, however, with their number/nucleation efficacy exponentially decreasing with time over a period of several 103 s at 190 °C. In contrast to many other polymers, oriented shish-like structures disappear well below the equilibrium melting temperature, allowing mild melting conditions to obtain an isotropic structure. The stability of the remaining structures in the melt seems to be caused/controlled by molecular interactions rather than by slow diffusion of the chain segments toward a random-coiled structure as the longest relaxation times (reptation) at about 180 °C are several orders of magnitude shorter than the observed lifetime of the ordered structures.
AB - Knowledge of the conditions required to obtain an isotropic melt of the polymer of interest, which before was subjected to shear and crystallization, is important for understanding and prediction of crystallization in polymer processing. In this work, the thermal stability of crystallization precursors of qualitatively different structures, namely, classical crystal remnants and oriented shish-like nuclei, is analyzed for poly(l-lactic acid) (PLLA). Shearing the melt at different rates leads to generation of shish-like and point-like nuclei which grow at identical temperature to crystals of similar stability/melting temperature. Analysis of the crystallization kinetics and of the semicrystalline morphology by differential scanning calorimetry and polarized-light optical microscopy, respectively, after subjecting the melt to different maximum temperatures, showed that disordering/isotropization of remnants of crystals, which melt close to 179 °C, occurs in a temperature window about 5-10 K higher than the melting temperature. Shish-like nuclei, generated at 135 °C during shearing the melt 10 s at 2 s-1, survive heating to a higher temperature than in the case of self-nuclei, however, with their number/nucleation efficacy exponentially decreasing with time over a period of several 103 s at 190 °C. In contrast to many other polymers, oriented shish-like structures disappear well below the equilibrium melting temperature, allowing mild melting conditions to obtain an isotropic structure. The stability of the remaining structures in the melt seems to be caused/controlled by molecular interactions rather than by slow diffusion of the chain segments toward a random-coiled structure as the longest relaxation times (reptation) at about 180 °C are several orders of magnitude shorter than the observed lifetime of the ordered structures.
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U2 - 10.1021/acsapm.2c01365
DO - 10.1021/acsapm.2c01365
M3 - Article
AN - SCOPUS:85139508268
SN - 2637-6105
VL - 4
SP - 7823
EP - 7833
JO - ACS Applied Polymer Materials
JF - ACS Applied Polymer Materials
IS - 10
ER -