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Chain orientation and defects in lamellar single crystals of syndiotactic polypropylene fractions

机译:间规聚丙烯级分的层状单晶的链取向和缺陷

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Sectorization is frequently observed in elongated rectangular single crystals of syndiotactic polypropylene (s-PP) grown from the melt in thin films. The crystals are bound laterally by {100} and {010} growth planes. The constituent sectors are readily observed because of a difference in thicknesses; specifically, the sectors bound by the {100} planes [the (100) growth sectors] are thicker than those bounded by the {010}planes [the (010) growth sectors]. Dark field (DF) transmission electron microscopy (TEM) was utilized to examine the chain orientation and lattice defects in the different growth sectors of s-PP single crystals. The (020) DF images exhibited pairs of bright streaks that are more or less perpendicular to the (100) planes and cross over the whole width of the (100) sectors. In the (200) DF images, the (100) sectors also exhibited similar but dimmer streaks than those in the (020) DF images. This suggests that the crystal c-axis orientation in the (100) crystal sectors undergoes a periodic change in inclination along both the longitudinal (parallel to the b-axis) and the transverse axis (parallel to the a-axis) directions of the single crystal. The ripples in the (100) sectors, previously observed in TEM, were also seen with atomic force microscopy as sinusoidal-like periodic height changes along the longitudinal axis direction at both room temperature and high temperatures. This periodic height change accounted for the pairs of bright streaks in the (020) DF images. The ripple formation was explained by lamellar thickening in the (010) sectors during crystal growth. This thickening process causes lateral contractions, which accumulate mainly along the longitudinal axis direction of the single crystal. On the other hand, the (020) DF images exhibited a relatively uniform brightness in the (010) sectors, while in the (200) DF images, several dark zones in the (010) sectors were more or less along the diagonal directions of the single crystal. This observation indicates that the crystal c-axis in these zones is slightly deviated from the (200) planarity due possibly to the lateral contraction in the (010) sectors. A regular Moire pattern in the (010) sectors was observed in the (020) DF images, and no Moire patterns were found in the (100) sectors. Again, this was presumably due to sinusoidal-like ripples, which substantially affect the crystal plane orientation with respect to the lamellar crystal normal. In the (200) DF images, only random Moire fringes could be found and, in particular, when the (010) and the (100) sectors overlapped. However, regular Moire fringes were observed continuously over both sectors in (220) DF images. [References: 23]
机译:在薄膜熔体中生长的间规聚丙烯(s-PP)的细长矩形单晶中经常观察到扇区化。晶体被{100}和{010}生长平面横向束缚。由于厚度的不同,很容易观察到组成部分。具体而言,受{100}平面约束的扇区[(100)增长扇区]比受{010}平面约束的扇区[[010]增长扇区]厚。暗场(DF)透射电子显微镜(TEM)用于检查s-PP单晶不同生长扇区中的链取向和晶格缺陷。 (020)DF图像显示出成对的亮条纹,这些亮条纹或多或少地垂直于(100)平面并跨越(100)扇区的整个宽度。在(200)DF图像中,(100)扇区也表现出与(020)DF图像相似但较暗的条纹。这表明(100)晶体扇区中的晶体c轴取向沿单个晶体的纵向(平行于b轴)和横向(平行于a轴)方向发生了周期性的倾斜变化。水晶。在原子力显微镜下,先前在TEM中观察到的(100)扇区中的波纹也被视为在室温和高温下沿纵轴方向呈正弦形的周期性高度变化。这种周期性的高度变化是(020)DF图像中成对的亮条纹的原因。晶体形成过程中(010)区域的层状增厚解释了波纹的形成。该增厚过程引起侧向收缩,该侧向收缩主要沿着单晶的纵轴方向累积。另一方面,(020)DF图像在(010)扇区中显示出相对均匀的亮度,而在(200)DF图像中,(010)扇区中的几个暗区或多或少沿着对角线方向单晶。该观察结果表明,由于(010)扇区中的横向收缩,这些区域中的晶体c轴稍微偏离(200)平面度。在(020)DF图像中观察到(010)扇区中有规则的莫尔图案,在(100)扇区中未发现莫尔图案。同样,这大概是由于正弦波状的波纹,这实际上影响了相对于层状晶体法线的晶体平面取向。在(200)DF图像中,只能找到随机的莫尔条纹,尤其是(010)和(100)扇区重叠时。但是,在(220)DF图像的两个扇区中连续观察到规则的莫尔条纹。 [参考:23]

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