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拉伸条件下聚四氟乙烯的相变行为及变形机制

Phase transition behavior and deformation mechanism of polytetrafluoroethylene under stretching.

作者信息

Luo Cong, Pei Jingke, Zhuo Wenyue, Niu Yanhua, Li Guangxian

机构信息

College of Polymer Science and Engineering, State Key Laboratory of Polymer Materials Engineering of China, Sichuan University Chengdu 610065 China

DEC Academy of Science and Technology Co, Ltd China.

出版信息

RSC Adv. 2021 Dec 14;11(63):39813-39820. doi: 10.1039/d1ra06333b. eCollection 2021 Dec 13.

DOI:10.1039/d1ra06333b
PMID:35494141
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9044566/
Abstract

The deformation mechanism and phase transition behavior of polytetrafluoroethylene (PTFE) under stretching conditions (25, 50, 100 °C) were investigated by using differential scanning calorimetry (DSC), small angle X-ray scattering (SAXS), and X-ray diffraction (XRD). Compared to the unstretched PTFE samples, stretching at all temperatures results in a reduced phase transition temperature (IV-I and II-IV). Above a critical strain (∼0.6), the decrease of phase transition temperature becomes more significant with the increasing strain. At higher stretching temperature, the value of the becomes smaller. By separating the recoverable ( ) and irreversible ( ) deformation, a similar (∼0.6) is found, beyond which the recoverable part remains basically unchanged while the unrecoverable part increases sharply. It is considered that as the strain reaches 0.6, both the untwisting of molecular chain and destroy of the crystal structure could occur, which leads to the increased plastic deformation of the system. Upon the strain is beyond 0.9, the degree of chain untwisting reaches the maximum, and a stable oriented fiber network structure forms, showing the phenomenon of elasticity enhancement. The deformation mechanism of PTFE changes from lamella slip at small strain to stretching induced formation of stable fibrils as evidenced by SEM and SAXS.

摘要

采用差示扫描量热法(DSC)、小角X射线散射(SAXS)和X射线衍射(XRD)研究了聚四氟乙烯(PTFE)在拉伸条件下(25、50、100℃)的变形机制和相变行为。与未拉伸的PTFE样品相比,在所有温度下拉伸都会导致相变温度降低(IV-I和II-IV)。在临界应变(约0.6)以上,相变温度的降低随着应变的增加而变得更加显著。在较高的拉伸温度下,临界应变的值变小。通过分离可恢复( )和不可逆( )变形,发现了类似的临界应变(约0.6),超过该临界应变后,可恢复部分基本保持不变,而不可恢复部分急剧增加。据认为,当应变达到0.6时,分子链的解缠和晶体结构的破坏都可能发生,这导致系统的塑性变形增加。当应变超过0.9时,链解缠程度达到最大,形成稳定的取向纤维网络结构,表现出弹性增强的现象。PTFE的变形机制从小应变下的片晶滑移转变为拉伸诱导形成稳定的原纤,扫描电子显微镜(SEM)和小角X射线散射(SAXS)证明了这一点。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/293f466f45db/d1ra06333b-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/fbb692180c01/d1ra06333b-f1.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/c1a7819df686/d1ra06333b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/9a8d52108c3a/d1ra06333b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/4531b900b3d0/d1ra06333b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/a049dac3f05f/d1ra06333b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/0a9c7fc4fa94/d1ra06333b-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/293f466f45db/d1ra06333b-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/fbb692180c01/d1ra06333b-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/10a7e9692247/d1ra06333b-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/c1a7819df686/d1ra06333b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/9a8d52108c3a/d1ra06333b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/4531b900b3d0/d1ra06333b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/a049dac3f05f/d1ra06333b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/0a9c7fc4fa94/d1ra06333b-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/206a/9044566/293f466f45db/d1ra06333b-f8.jpg

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