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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 = 70-140 °C). Active deformation mechanisms have been identified and compared for two different deformation modes-uniaxial drawing and plane-strain compres...
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Published in: | Polymers 2021-12, Vol.13 (24), p.4432 |
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description | The ability of PLLA, either amorphous or semicrystalline, to plastic deformation to large strain was investigated in a wide temperature range (T
= 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
= 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
= 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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= 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
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= 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
= 115-140 °C), the α→β crystal transformation was additionally observed, leading to the formation of a small fraction of β crystals.</description><subject>Crystal structure</subject><subject>Crystallization</subject><subject>Crystallography</subject><subject>Crystals</subject><subject>Deformation</subject><subject>Deformation mechanisms</subject><subject>Ductile-brittle transition</subject><subject>High temperature</subject><subject>Mesophase</subject><subject>Plane strain</subject><subject>Plastic deformation</subject><subject>Plastic flow</subject><subject>Polymers</subject><subject>Slip</subject><subject>Strain analysis</subject><subject>Temperature</subject><subject>True strain</subject><issn>2073-4360</issn><issn>2073-4360</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNpdkUtLxDAUhYMoKjpLt1Jwo4tqXk2TjSDjEwYcUHdCyKSJRtpkTFrRf2-Ko6hZ3ATud0_u4QCwh-AxIQKeLEP70SGCKaUEr4FtDGtSUsLg-q_3Fpik9ALzoRVjqN4EW4QKBgWn2-Dx3NgQO9W74Itgi3lWLNuyVbp3TaF0Lofz2ezsqBh8Y2Lx4J16d6ot7o1P44zyTTFvlTflXR-V88U0dMto0tjcBRtWtclMVvcOeLi8uJ9el7Pbq5vp2azUFFV9abgVmnBc03pBEYGVUIpVUONFw6kQDbdIY8UoF9hYiixc1JZpVVNOMBawIjvg9Et3OSw602jj8yqtXEbXqfghg3Lyb8e7Z_kU3iSvIeeMZIHDlUAMr4NJvexc0qYdfYUhScxQhTJaj38d_ENfwhB9tjdSmFPMK5yp8ovSMaQUjf1ZBkE5Rif_RJf5_d8OfujvoMgnYLGUFA</recordid><startdate>20211217</startdate><enddate>20211217</enddate><creator>Vozniak, Alina</creator><creator>Bartczak, Zbigniew</creator><general>MDPI AG</general><general>MDPI</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0003-0514-9106</orcidid><orcidid>https://orcid.org/0000-0002-4023-0375</orcidid></search><sort><creationdate>20211217</creationdate><title>Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression</title><author>Vozniak, Alina ; Bartczak, Zbigniew</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c415t-e8f9c382747b413059aa650c2bd8499d8f1c2a64892ef41f0b7f6ca7483229053</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Crystal structure</topic><topic>Crystallization</topic><topic>Crystallography</topic><topic>Crystals</topic><topic>Deformation</topic><topic>Deformation mechanisms</topic><topic>Ductile-brittle transition</topic><topic>High temperature</topic><topic>Mesophase</topic><topic>Plane strain</topic><topic>Plastic deformation</topic><topic>Plastic flow</topic><topic>Polymers</topic><topic>Slip</topic><topic>Strain analysis</topic><topic>Temperature</topic><topic>True strain</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Vozniak, Alina</creatorcontrib><creatorcontrib>Bartczak, Zbigniew</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>Materials Science Database</collection><collection>Materials science collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Polymers</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Vozniak, Alina</au><au>Bartczak, Zbigniew</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression</atitle><jtitle>Polymers</jtitle><addtitle>Polymers (Basel)</addtitle><date>2021-12-17</date><risdate>2021</risdate><volume>13</volume><issue>24</issue><spage>4432</spage><pages>4432-</pages><issn>2073-4360</issn><eissn>2073-4360</eissn><abstract>The ability of PLLA, either amorphous or semicrystalline, to plastic deformation to large strain was investigated in a wide temperature range (T
= 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
= 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
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subjects | Crystal structure Crystallization Crystallography Crystals Deformation Deformation mechanisms Ductile-brittle transition High temperature Mesophase Plane strain Plastic deformation Plastic flow Polymers Slip Strain analysis Temperature True strain |
title | Deformation of Poly-l-lactid acid (PLLA) under Uniaxial Tension and Plane-Strain Compression |
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