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Elongational Flow of Polymer Melts at Constant Strain Rate, Constant Stress and Constant Force

机译:聚合物伸长流动以恒定应变速率,恒定应力和恒定力熔化

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Characterization of polymer melts in elongational flow is typically performed at constant elongational rate or rarely at constant tensile stress conditions. One of the disadvantages of these deformation modes is that they are hampered by the onset of "necking" instabilities according to the Considere criterion. Experiments at constant tensile force have been performed even more rarely, in spite of the fact that this deformation mode is free from necking instabilities and is of considerable industrial relevance as it is the correct analogue of steady fiber spinning. It is the objective of the present contribution to present for the first time a full experimental characterization of a long-chain branched polyethylene melt in elongational flow. Experiments were performed at constant elongation rate, constant tensile stress and constant tensile force by use of a Sentmanat Extensional Rheometer (SER) in combination with an Anton Paar MCR301 rotational rheometer. The accessible experimental window and experimental limitations are discussed. The experimental data are modelled by using the Wagner I model. Predictions of the steady-start elongational viscosity in constant strain rate and creep experiments are found to be identical, albeit only by extrapolation of the experimental data to Hencky strains of the order of 6. For constant stress experiments, a minimum in the strain rate and a corresponding maximum in the elongational viscosity is found at a Hencky strain of the order of 3, which, although larger than the steady-state value, follows roughly the general trend of the steady-state elongational viscosity. The constitutive analysis also reveals that constant tensile force experiments indicate a larger strain hardening potential than seen in constant elongation rate or constant tensile stress experiments. This may be indicative of the effect of necking under constant elongation rate or constant tensile stress conditions according to the Considere criterion.
机译:聚合物熔体在延长流动中的表征通常在恒定的伸缩速率下或很少在恒定的拉应力条件下进行。这些变形模式的一个缺点是,根据指导标准,它们被“缩颈”不稳定性的发作所阻碍。尽管这种变形模式没有缩颈,但由于这种变形模式不具有相当大的纤维纺丝而具有相当大的工业相关性,但仍然更少地进行了恒定拉力的实验。本发明的目的是本贡献于第一次出现长链支化聚乙烯熔体在延长流动中的全实验表征。通过使用与ANTON PAAR MCR301旋转流变仪组合的Sentmanat延伸流变仪(Ser)以恒定的伸长率,恒定拉伸应力和恒定拉伸力进行实验。讨论了可访问的实验窗口和实验局限性。通过使用WAGNER I模型建模实验数据。发现恒定应变速率和蠕变实验中稳态伸长率粘度的预测是相同的,尽管仅通过将实验数据推断为6.对于恒定应力实验,但恒定应力实验的最小值和伸长粘度的相应最大值以3的量级为3,虽然大于稳态值,但大致呈稳态伸缩粘度的一般趋势。本构体分析还揭示了恒定的拉力实验表明,恒定的伸长率或恒定拉应力实验中的较大应变硬化电位。这可以指示根据指导标准在恒定伸长率或恒定拉应力条件下的颈缩的影响。

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