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Confined crystallization and morphology of melt segregated PLLA-b-PE and PLDA-b-PE diblock copolymers

机译:熔融分离的PLLA-b-PE和PLDA-b-PE二嵌段共聚物的密闭结晶和形态

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The crystallization behavior of strongly segregated diblock copolymers composed of polyethylene (PE) and poly(L-lactide) or racemic poly(lactide) (PLA) blocks has been investigated by differential scanning calorimetry (DSC), small-angle X-ray scattering (SAXS), wide-angle X-ray scattering (WAXS), and transmission electron microscopy (TEM). In both systems the crystallization of PE block was confined within the preexisting lamellar domain. In the double-crystalline PLLA-b-PE, coincident crystallization of PLLA and PE blocks was observed during cooling process because the crystallization rate of the PLLA block was retarded by the covalent linkage with the PE block. When the PLLA block was self-nucleated, a complete separation of the crystallization process of both blocks was achieved. Polarized optical microscopy confirmed that neither PLLA nor PE blocks could form spherulites in view of the large segregation strength that effectively confined the crystallization within the lamellar microdomains. High-speed DSC was applied to reduce reorganization during the scan so that values closer to the equilibrium melting points (T-m degrees), employing the Hoffman-Weeks treatment, could be obtained for PLLA. The T-m degrees for the PLLA block was depressed as compared to homo-PLLA by confinement effects. The crystallization of the PE block within the amorphous-crystalline PLDA-b-PE was strictly confined, and the microdomain morphology established in the melt state was essentially unperturbed, regardless of whether the crystallization occurred when the PLDA block was glassy or rubbery (hard or soft confinement). In the case of the double-crystalline PLLA-b-PE system, the crystallizations of both PE and PLLA blocks were also effectively confined within the respective lamellar microdomains, irrespective of which is the leading crystallizing component prescribed by the crystallization history. The confinement effect was a consequence of the large segregation strength coupled with the solidification of the microdomains of the leading crystallizing component, which subsequently imposed a hard confinement effect on the crystallization of the second block. TEM revealed the ordered lamellar morphology, and in one case the crystalline lamellae of the PE block were visualized within the microphase-separated lamellae due to an isothermal crystallization pretreatment.
机译:已经通过差示扫描量热法(DSC),小角度X射线散射法研究了由聚乙烯(PE)和聚(L-丙交酯)或外消旋聚(丙交酯)(PLA)嵌段组成的强分离二嵌段共聚物的结晶行为。 SAXS),广角X射线散射(WAXS)和透射电子显微镜(TEM)。在这两个系统中,PE嵌段的结晶都被限制在预先存在的层状结构域内。在双晶PLLA-b-PE中,在冷却过程中观察到了PLLA和PE嵌段的同时结晶,这是因为PLLA嵌段的结晶速率由于与PE嵌段的共价键合而受阻。当PLLA嵌段是自成核的时,两个嵌段的结晶过程完全分离。偏振光学显微镜证实,鉴于大的分离强度有效地限制了层状微区中的结晶,PLLA和PE嵌段均不能形成球晶。应用高速DSC来减少扫描过程中的重组,以便采用Hoffman-Weeks处理,可以为PLLA获得更接近平衡熔点(T-m度)的值。通过限制效应,与同质PLLA相比,PLLA块的T-m度降低了。严格限制了PE嵌段在无定形PLDA-b-PE晶体中的结晶,并且在熔融状态下建立的微区形态基本上不受干扰,无论PLDA嵌段是玻璃态还是橡胶态(硬或软禁闭)。在双晶PLLA-b-PE系统的情况下,PE和PLLA嵌段的结晶也有效地限制在各自的层状微区中,而不管结晶历史所规定的主要结晶成分是什么。该限制作用是由于较大的偏析强度以及前导结晶组分的微区的固化而导致的,其随后对第二嵌段的结晶施加了硬限制作用。 TEM揭示了有序的层状形态,在一种情况下,由于等温结晶预处理,在微相分离的片层中可以看到PE嵌段的结晶片层。

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