Heterogeneous Stress Distribution and Hierarchical Structure in the Highly Oriented Nylon 6 Strings Annealed at Various Temperatures to Evaluate the True Crystallite Modulus
Heterogeneous Stress Distribution and Hierarchical Structure in the Highly Oriented Nylon 6 Strings Annealed at Various Temperatures to Evaluate the True Crystallite Modulus
复制标题
在不同温度下退火的高取向尼龙 6 线中的不均匀应力分布和层次结构,以评估真实的微晶模量
DOI:
10.1021/acs.macromol.1c00142
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发表时间:
2021
期刊:
影响因子:
5.5
通讯作者:
Tashiro Kohji
中科院分区:
文献类型:
--
作者:
Kummara Sreenivas;Tashiro Kohji
The apparent crystallite modulusEcappalong the chain axis has been measured by the X-ray diffraction method for a series of melt-drawn nylon 6 strings annealed at various temperatures under tension, where “apparent” means Young’s modulus obtained under the assumption of the homogeneous stress distribution or the assumption of the equality between the crystalline stress and the stress of the bulk sample. TheEcappdecreased drastically from 160 GPa of the original unannealed sample to 60 GPa for the sample annealed in a temperature region of 30–180 °C (region I) and then increased steeply up to 230 GPa by the annealing in 180–220 °C (region II). TheEbulkor Young’s modulus of the bulk sample was about 3.5 GPa and did not change very much in region I, and it increased to 5 GPa by annealing in region II. In order to interpret the observed change inEcappandEbulkfrom the structural point of view, various experimental data have been collected for all of the samples used here on the basis of the wide-angle and small-angle X-ray scattering, the polarized infrared (IR) spectra, and the thermal analysis, from which the unit cell parameters, the anisotropic crystallite size, the degree of crystallinity, the degree of chain orientation in the crystalline and amorphous regions, the long period and averaged thickness of the stacked lamellae, and so forth have been determined. The thus-derived structural features may be described as follows: the original melt-drawn sample consisted of the highly oriented crystalline phase and the mechanically strained and relatively highly oriented amorphous phase containing a small amount of the taut tie chains. The heat treatment in region I caused an increase of these tie chains with the chain orientation kept unchanged in both of the crystalline and amorphous regions. The annealing in region II induced the remarkable structural evolution of the larger crystallites with the more regularly packed and more highly extended chains. The mechanical series–parallel model was introduced, and the parameters (pandq) were chosen suitably to give a satisfactorily good reproduction of the observedEcapp. The annealing effect on these parameters was found to correspond well to the structural evolution revealed by the X-ray and IR data analysis. The finally obtained maximalEctrueor the true Young’s modulus along the chain axis was about 290 GPa for the sample annealed immediately below the melting point, which is closer to but slightly lower than the value 312 GPa predicted theoretically for the fully extended nylon 6 chains in the crystal lattice.