Cargando…

Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between

[Image: see text] The enantiomeric ratio is a key factor affecting the crystallization behavior and morphology of poly-l-lactide/poly-d-lactide (PLLA/PDLA) blends. Despite a number of studies on crystallization of nonequimolar PLLA/PDLA blends, a full picture of the effect of the L/D ratio is still...

Descripción completa

Detalles Bibliográficos
Autores principales: Cui, Jiaming, Yang, Shu-Gui, Zhang, Ruibin, Cao, Yu, Wang, Yubo, Zeng, Xiangbing, Liu, Feng, Ungar, Goran
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10653275/
https://www.ncbi.nlm.nih.gov/pubmed/38024153
http://dx.doi.org/10.1021/acs.macromol.3c01815
_version_ 1785147759709388800
author Cui, Jiaming
Yang, Shu-Gui
Zhang, Ruibin
Cao, Yu
Wang, Yubo
Zeng, Xiangbing
Liu, Feng
Ungar, Goran
author_facet Cui, Jiaming
Yang, Shu-Gui
Zhang, Ruibin
Cao, Yu
Wang, Yubo
Zeng, Xiangbing
Liu, Feng
Ungar, Goran
author_sort Cui, Jiaming
collection PubMed
description [Image: see text] The enantiomeric ratio is a key factor affecting the crystallization behavior and morphology of poly-l-lactide/poly-d-lactide (PLLA/PDLA) blends. Despite a number of studies on crystallization of nonequimolar PLLA/PDLA blends, a full picture of the effect of the L/D ratio is still lacking. Here, we put the two enantiomers in contact and allow interdiffusion above the melting point of the stereocomplex crystal (SC) to prepare samples with a continuously changing L/D ratio from enantiopure PLLA (ratio 0/100) to enantiopure PDLA (100/0). Using polarized optical microscopy, atomic force microscopy, and microbeam X-ray diffraction, the continuous spectrum of morphologies and phase behaviors across the contact zone is investigated. The blend morphology shows clear evidence of “poisoning by purity” of SC crystallization at all blend compositions. The low birefringence of the 50/50 SC is found to be due to the meandering of broken edge-on lamellae. Its further decrease to near zero as L/D deviates further away from 50/50 is explained by transition from radial edge-on lamellae to fully random meandering lamellae, then to mixed flat-on lamellae, and finally to submicron-sized axialites. In comparison with the smooth and straight homocrystal (HC) lamellae of pure enantiomers, the lamellae in the blends often have serrated edges caused by pinning by rejected excess enantiomer acting as an impurity during lamellar growth. A feature of the binary phase diagram is pure enantiomers acting as an impurity to the SC and counter-enantiomer acting as an impurity to homocrystallization of the enantiomers. Crystallization was found to be most suppressed at 99% enantiomeric purity, where the amount of the counter-enantiomer is insufficient for creation of SC nuclei and HC growth is inhibited by the small amount of the enantio-impurity. These and other intriguing results are less likely to be noticed without the continuous composition gradient of the contact sample.
format Online
Article
Text
id pubmed-10653275
institution National Center for Biotechnology Information
language English
publishDate 2023
publisher American Chemical Society
record_format MEDLINE/PubMed
spelling pubmed-106532752023-11-16 Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between Cui, Jiaming Yang, Shu-Gui Zhang, Ruibin Cao, Yu Wang, Yubo Zeng, Xiangbing Liu, Feng Ungar, Goran Macromolecules [Image: see text] The enantiomeric ratio is a key factor affecting the crystallization behavior and morphology of poly-l-lactide/poly-d-lactide (PLLA/PDLA) blends. Despite a number of studies on crystallization of nonequimolar PLLA/PDLA blends, a full picture of the effect of the L/D ratio is still lacking. Here, we put the two enantiomers in contact and allow interdiffusion above the melting point of the stereocomplex crystal (SC) to prepare samples with a continuously changing L/D ratio from enantiopure PLLA (ratio 0/100) to enantiopure PDLA (100/0). Using polarized optical microscopy, atomic force microscopy, and microbeam X-ray diffraction, the continuous spectrum of morphologies and phase behaviors across the contact zone is investigated. The blend morphology shows clear evidence of “poisoning by purity” of SC crystallization at all blend compositions. The low birefringence of the 50/50 SC is found to be due to the meandering of broken edge-on lamellae. Its further decrease to near zero as L/D deviates further away from 50/50 is explained by transition from radial edge-on lamellae to fully random meandering lamellae, then to mixed flat-on lamellae, and finally to submicron-sized axialites. In comparison with the smooth and straight homocrystal (HC) lamellae of pure enantiomers, the lamellae in the blends often have serrated edges caused by pinning by rejected excess enantiomer acting as an impurity during lamellar growth. A feature of the binary phase diagram is pure enantiomers acting as an impurity to the SC and counter-enantiomer acting as an impurity to homocrystallization of the enantiomers. Crystallization was found to be most suppressed at 99% enantiomeric purity, where the amount of the counter-enantiomer is insufficient for creation of SC nuclei and HC growth is inhibited by the small amount of the enantio-impurity. These and other intriguing results are less likely to be noticed without the continuous composition gradient of the contact sample. American Chemical Society 2023-10-27 /pmc/articles/PMC10653275/ /pubmed/38024153 http://dx.doi.org/10.1021/acs.macromol.3c01815 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Cui, Jiaming
Yang, Shu-Gui
Zhang, Ruibin
Cao, Yu
Wang, Yubo
Zeng, Xiangbing
Liu, Feng
Ungar, Goran
Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title_full Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title_fullStr Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title_full_unstemmed Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title_short Continuous Spectrum of Morphologies and Phase Behavior across the Contact Zone from Poly(l-lactide) to Poly(d-lactide): Stereocomplex, Homocrystal, and Between
title_sort continuous spectrum of morphologies and phase behavior across the contact zone from poly(l-lactide) to poly(d-lactide): stereocomplex, homocrystal, and between
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10653275/
https://www.ncbi.nlm.nih.gov/pubmed/38024153
http://dx.doi.org/10.1021/acs.macromol.3c01815
work_keys_str_mv AT cuijiaming continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT yangshugui continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT zhangruibin continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT caoyu continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT wangyubo continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT zengxiangbing continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT liufeng continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween
AT ungargoran continuousspectrumofmorphologiesandphasebehavioracrossthecontactzonefrompolyllactidetopolydlactidestereocomplexhomocrystalandbetween