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Orientation distribution functions obtained via polarized Raman spectroscopy of poly(ethylene terephthalate) fibers

机译:聚对苯二甲酸乙二醇酯纤维的偏振拉曼光谱获得的取向分布函数

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摘要

Polarized Raman microspectroscopy was used to analyze uniaxially oriented fibers of poly(ethylene terephthalate) (PET). A full analysis of bands at 1616, 998, and 1096 cm(-1) is reported for cylindrically symmetric PET fibers. Average orientation and crystal orientation are obtained from the 1616 and 998 cm(-1) band, respectively. Although both the 1096 and the 998 cm(-1) bands are related to the crystallinity, the second Legendre polynomial of the 1096 cm(-1) band, P-2,P-1096, is substantially smaller than for the 998 cm(-1) band, P-2,P-998. In addition, P-2,P-1096 is not related to the birefringence of the samples, and there is no simple relationship between P-2,P-1096 and P-2,P-998. The orientation distribution functions (ODFs) for these vibrations were obtained by assuming a Gaussian distribution with a tilt angle relative to the fiber axis and specific to each vibration. The 1616 cm(-1) band has a tilt angle of 23 +/- 4degrees, and the ODF becomes narrower as molecular orientation increases. The 998 cm(-1) band has a tilt angle of approximately 0degrees, and the ODF is always very narrow. On the other hand, the tilt angle of the 1096 cm(-1) band increases, and the ODF becomes narrower as the molecular orientation increases. However, because of the large tilt angle, P-2 for this band decreases as the molecular orientation increases. [References: 29]
机译:偏振拉曼光谱用于分析聚对苯二甲酸乙二醇酯(PET)的单轴取向纤维。报告了对圆柱形对称PET纤维在1616、998和1096 cm(-1)处的带的完整分析。平均取向和晶体取向分别从1616和998 cm(-1)波段获得。尽管1096和998 cm(-1)谱带都与结晶度有关,但1096 cm(-1)谱带的第二勒让德多项式P-2,P-1096远小于998 cm(-1)。 -1)频段,P-2,P-998。另外,P-2,P-1096与样品的双折射无关,在P-2,P-1096和P-2,P-998之间没有简单的关系。这些振动的取向分布函数(ODF)是通过假设高斯分布而获得的,其中高斯分布相对于纤维轴具有倾斜角,并且特定于每种振动。 1616 cm(-1)带的倾斜角为23 +/- 4度,并且ODF随着分子方向的增加而变窄。 998 cm(-1)波段的倾斜角度约为0度,ODF始终很窄。另一方面,1096 cm(-1)谱带的倾斜角增加,并且随着分子取向的增加,ODF变窄。然而,由于大的倾斜角,该带的P-2随着分子取向的增加而降低。 [参考:29]

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