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首页> 外文期刊>Polymer: The International Journal for the Science and Technology of Polymers >Tensile study of melt-spun poly(3-hydroxybutyrate) P3HB fibers: Reversible transformation of a highly oriented phase
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Tensile study of melt-spun poly(3-hydroxybutyrate) P3HB fibers: Reversible transformation of a highly oriented phase

机译:熔纺聚(3-羟基丁酸酯)P3HB纤维的拉伸研究:高度取向相的可逆变换

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摘要

Poly-3-hydroxybutyrate (P3HB) typically crystallizes into the orthorhombic alpha-form. The additional intense and rather broad equatorial reflection in wide-angle X-ray diffraction (WAXD) patterns seen in our melt-spun P3HB fibers cannot be attributed to the a-form crystals. We propose that a non-crystalline mesophase, which consists of disordered but highly oriented and stretched molecules located between alpha-crystals, leads to the observed broad equatorial reflection. We show that the transformation of this mesophase from and into the alpha-form phase is partially reversible under cyclic tensile loading. Structure factor calculations, which are based on atomic positions from molecular dynamics simulations of a set of stretched P3HB molecules, support this model. The WAXD patterns were analyzed with azimuthal, radial, equatorial and meridional scans and the changes in the crystal orientation, changes in the percentages of individual phases and changes in the alpha-crystal lattice spacings were analyzed as a function of the applied tension. Changes in long spacings, crystal sizes and coherence lengths under cyclic loading were determined with small-angle X-ray scattering (SAXS) measurements. The long spacing between alpha-crystals increases when tensile stress is applied and it snaps back to the original spacing when the tensile stress is released.
机译:聚-3-羟基丁酸盐(P3HB)通常在正交α形式中结晶。在我们的熔融纺丝P3HB纤维中看到的广角X射线衍射(WAXD)图案中的额外强烈且相当较大的赤道反射不能归因于A形晶体。我们提出了一种非结晶的中间相,由位于α-晶体之间的无序但高度取向和拉伸分子组成,导致观察到的宽赤道反射。我们表明,在循环拉伸载荷下,将该中间相的转化为α-型相的α-型相。结构因子计算,基于来自一组拉伸的P3HB分子的分子动力学模拟的原子位置,支持该模型。通过方位角,径向,赤道和优异的扫描分析蜡状图案,并且作为施加张力的函数分析了晶体取向的变化,各个相的百分比和α晶格间距的变化的变化。通过小角度X射线散射(SAXS)测量测定循环加载下的长间距,晶体尺寸和相干长度的变化。当施加拉伸应力时,α-晶体之间的长间距增加,并且当释放拉伸应力时,将其捕回原始间隔。

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