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Polymer crystalline texture controlled through film blowing and block copolymerization.

机译:通过吹膜和嵌段共聚来控制聚合物的晶体质地。

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Polymer properties can be manipulated through processing or chemical modification. Both methods are explored here, by (a) elucidating the origin of directional tear behavior in polyethylene (PE) films processed under different conditions, and (b) synthesizing new block copolymers, whose architectures permit precise control over crystal thickness and melting temperature.; Directional tear in films of PE and its copolymers was traced to the orientation imparted during film blowing, quantified through x-ray scattering. The blow-up ratio (BUR) was the most significant process parameter controlling crystal orientation. The Keller-Machin I structure was observed in low-density polyethylene (LDPE) films, which tore preferentially in the transverse direction (TD). Conversely, the Keller-Machin II structure was observed in ethylene-methacrylic acid copolymer films at low BUR, which also tore TD, but the orientation rotated 90° at high BUR, leading to preferred tear in the machine direction (MD). High-density and linear low-density PE films also exhibited the Keller-Machin I structure (as in LDPE) but tore either along MD (HDPE) or isotropically (LLDPE). These differences in tear behavior between chemically similar but architecturally distinct polymers, differing greatly in the type and level of branching, stem from intercrystallite tie molecules.; In the second area, crystalline-amorphous diblock copolymers were synthesized through ring-opening metathesis polymerization and subsequent hydrogenation, where the amorphous block was hydrogenated poly(ethylidene norbornene), hPEN, and the crystalline block was either hydrogenated polycyclopentene, hPCP (identical to HDPE) or hydrogenated polynorbornene, hPN. Acyclic metathesis discovered during the PCP synthesis focused the study on block copolymers containing hPN, which is atactic yet highly crystalline. The hPN crystal structure was solved as monoclinic-β (space group C2/c), with a = 6.936 Å, b = 9.596 Å, c = 12.420 Å, and β = 130.7°. hPN/hPEN diblocks of constant crystalline block length and different amorphous block lengths permitted a direct test of theoretical scaling laws based on the premise of an equilibrium degree of crystal chain folding. Stable chain folding induced by the amorphous block was confirmed, and the theoretical scaling laws were generally verified, though integral chain folding by the crystalline block superimposes a discreteness on the continuous domain scaling predictions. As the amorphous block length increased, producing thinner crystals, the melting point decreased commensurably. The melting point was also influenced by the monomeric and polymeric endgroups attached to the crystallizable block, through the crystal surface energy.
机译:可以通过加工或化学改性来控制聚合物的性能。 (a)阐明在不同条件下加工的聚乙烯(PE)膜中定向撕裂行为的起因,以及(b)合成新的嵌段共聚物,其结构可以精确控制晶体厚度和熔融温度,从而探索了这两种方法。 PE及其共聚物薄膜的定向撕裂可追溯到吹膜过程中赋予的取向,并通过X射线散射进行定量。吹胀比(BUR)是控制晶体取向的最重要的工艺参数。在低密度聚乙烯(LDPE)薄膜中观察到Keller-Machin I结构,该薄膜优先沿横向(TD)撕裂。相反,在低BUR的乙烯-甲基丙烯酸共聚物薄膜中观察到Keller-Machin II结构,该薄膜也撕裂了TD,但在高BUR时取向旋转了90°,导致在纵向(MD)上出现了较好的撕裂。高密度和线性低密度PE膜也表现出Keller-Machin I结构(如LDPE),但沿MD(HDPE)或各向同性(LLDPE)撕裂。化学上相似但结构上不同的聚合物之间的撕裂行为差异,在分支类型和支链水平上差异很大,这是由于晶间键合分子引起的。在第二区域中,通过开环易位聚合反应和随后的氢化反应,合成了晶体-无定形二嵌段共聚物,其中无定形嵌段是氢化聚(亚乙基降冰片烯),hPEN,结晶嵌段是氢化了聚环戊烯,hPCP(与HDPE相同) )或氢化聚降冰片烯,hPN。在PCP合成过程中发现的无环复分解研究集中在含有hPN的嵌段共聚物上,hPN是无规的但高度结晶。将hPN晶体结构解析为单斜晶β(空间群C2 / c ),其中 a = 6.936Å, b = 9.596Å, = 12.420Å,β= 130.7°。恒定晶体块长度和不同无定形块长度的hPN / hPEN二嵌段可以在平衡晶体链折叠度的前提下直接测试理论比例定律。确认了由非晶嵌段引起的稳定链折叠,并且尽管由结晶嵌段进行的整体链折叠在连续畴尺寸预测上叠加了离散性,但是通常验证了理论上的定标律。随着无定形嵌段长度的增加,产生较薄的晶体,熔点相应降低。熔点还受晶体表面能的影响而附着在可结晶嵌段上的单体和聚合物端基的影响。

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