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Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression

The ability of PLLA, either amorphous or semicrystalline, to plastic deformation to large strain was investigated in a wide temperature range (T(d) = 70–140 °C). Active deformation mechanisms have been identified and compared for two different deformation modes—uniaxial drawing and plane-strain comp...

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Autores principales: Vozniak, Alina, Bartczak, Zbigniew
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8708863/
https://www.ncbi.nlm.nih.gov/pubmed/34960984
http://dx.doi.org/10.3390/polym13244432
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author Vozniak, Alina
Bartczak, Zbigniew
author_facet Vozniak, Alina
Bartczak, Zbigniew
author_sort Vozniak, Alina
collection PubMed
description The ability of PLLA, either amorphous or semicrystalline, to plastic deformation to large strain was investigated in a wide temperature range (T(d) = 70–140 °C). Active deformation mechanisms have been identified and compared for two different deformation modes—uniaxial drawing and plane-strain compression. The initially amorphous PLLA was capable of significant deformation in both tension and plane-strain compression. In contrast, the samples of crystallized PLLA were found brittle in tensile, whereas they proved to be ductile and capable of high-strain deformation when deformed in plane-strain compression. The main deformation mechanism identified in amorphous PLLA was the orientation of chains due to plastic flow, followed by strain-induced crystallization occurring at the true strain above e = 0.5. The oriented chains in amorphous phase were then transformed into oriented mesophase and/or oriented crystals. An upper temperature limit for mesophase formation was found below T(d) = 90 °C. The amount of mesophase formed in this process did not exceed 5 wt.%. An additional mesophase fraction was generated at high strains from crystals damaged by severe deformation. After the formation of the crystalline phase, further deformation followed the mechanisms characteristic for the semicrystalline polymer. Interlamellar slip supported by crystallographic chain slip has been identified as the major deformation mechanism in semicrystalline PLLA. It was found that the contribution of crystallographic slip increased notably with the increase in the deformation temperature. The most probable active crystallographic slip systems were (010)[001], (100)[001] or (110)[001] slip systems operating along the chain direction. At high temperatures (T(d) = 115–140 °C), the α→β crystal transformation was additionally observed, leading to the formation of a small fraction of β crystals.
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spelling pubmed-87088632021-12-25 Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression Vozniak, Alina Bartczak, Zbigniew Polymers (Basel) Article The ability of PLLA, either amorphous or semicrystalline, to plastic deformation to large strain was investigated in a wide temperature range (T(d) = 70–140 °C). Active deformation mechanisms have been identified and compared for two different deformation modes—uniaxial drawing and plane-strain compression. The initially amorphous PLLA was capable of significant deformation in both tension and plane-strain compression. In contrast, the samples of crystallized PLLA were found brittle in tensile, whereas they proved to be ductile and capable of high-strain deformation when deformed in plane-strain compression. The main deformation mechanism identified in amorphous PLLA was the orientation of chains due to plastic flow, followed by strain-induced crystallization occurring at the true strain above e = 0.5. The oriented chains in amorphous phase were then transformed into oriented mesophase and/or oriented crystals. An upper temperature limit for mesophase formation was found below T(d) = 90 °C. The amount of mesophase formed in this process did not exceed 5 wt.%. An additional mesophase fraction was generated at high strains from crystals damaged by severe deformation. After the formation of the crystalline phase, further deformation followed the mechanisms characteristic for the semicrystalline polymer. Interlamellar slip supported by crystallographic chain slip has been identified as the major deformation mechanism in semicrystalline PLLA. It was found that the contribution of crystallographic slip increased notably with the increase in the deformation temperature. The most probable active crystallographic slip systems were (010)[001], (100)[001] or (110)[001] slip systems operating along the chain direction. At high temperatures (T(d) = 115–140 °C), the α→β crystal transformation was additionally observed, leading to the formation of a small fraction of β crystals. MDPI 2021-12-17 /pmc/articles/PMC8708863/ /pubmed/34960984 http://dx.doi.org/10.3390/polym13244432 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Vozniak, Alina
Bartczak, Zbigniew
Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title_full Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title_fullStr Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title_full_unstemmed Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title_short Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression
title_sort deformation of poly-l-lactid acid (plla) under uniaxial tension and plane-strain compression
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8708863/
https://www.ncbi.nlm.nih.gov/pubmed/34960984
http://dx.doi.org/10.3390/polym13244432
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