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Properties of random and block copolymers of butadiene and styrene. II. Melt flow

机译:丁二烯和苯乙烯的无规共聚物和嵌段共聚物的性质。II. 熔体流动

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AbstractFlow curves, log (rate of shear) versus log (shear stress), as functions of temperature were obtained for several butadiene‐styrene copolymers of fixed (25) styrene content, differing in monomer sequence distribution. A random copolymer of constant composition along the polymer chain and narrow molecular weight distribution (MWD) exhibited behavior similar to linear, narrow MWD polybutadienes; the flow was Newtonian at low shear stresses, and the flow curves for various temperatures were accurately superimposable by a shift along the log (shear rate) axis. In a random copolymer varying in composition along the polymer chain, non‐Newtonian behavior was more pronounced, and temperature‐shear rate superposition did not succeed, a trend further perpetuated in copolymer of a single long styrene block sequence. The latter resemble branched polymers, as would be expected from association of the styrene blocks. With two styrene blocks, association produces network structures below the glass transition of polystyrene with consequent loss of flow. Disruption of these associations aboveTg(styrene) imparts the greatest thermoplasticity to these elastomers. There is evidence, however, that some of the associations persist at temperatures well in excess ofTg(sty
机译:摘要几种苯乙烯含量固定(25%)的丁二烯-苯乙烯共聚物,单体序列分布不同,获得了对数(剪切速率)与对数(剪切应力)作为温度函数的流动曲线。沿聚合物链和窄分子量分布(MWD)具有恒定成分的无规共聚物表现出与线性窄MWD聚丁二烯相似的行为;在低剪切应力动是牛顿的,不同温度下的流动曲线可以通过沿对数(剪切速率)轴的位移精确叠加。在沿聚合物链的成分变化的随机共聚物中,非牛顿行为更为明显,并且温度-剪切速率叠加没有成功,这一趋势在单个长苯乙烯嵌段序列的共聚物中进一步延续。后者类似于支链聚合物,正如苯乙烯嵌段的结合所预期的那样。对于两个苯乙烯嵌段,缔合在聚苯乙烯的玻璃化转变下方产生网络结构,从而产生流动损失。上述Tg(苯乙烯)上述这些缔合的破坏赋予了这些弹性体最大的热塑性。然而,有证据表明,一些关联在远远超过Tg(sty)的温度下持续存在

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