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Solid phase rheology of a thermotropic nematic polymer.

机译:热塑性向列型聚合物的固相流变学。

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We have performed a series of experiments at finite strain which indicate that a liquid crystalline copolyester, Vectra, has a region of viscoelastic behavior where all strain is recoverable and the stress response is approximately linear. We also find that at strains outside this region the polymer responds as a nonlinear viscoelastic material, and not all of the strain is recoverable. We have attempted to construct a simple model to describe this behavior.; At strains of 0.005 or greater the material clearly behaves as a nonlinear viscoelastic-viscoplastic material. The most readily visible aspect of this behavior is the development of non-recoverable strain and its dependence on the strain history. The plastic strain is a function of the applied strain. Moreover, short duration loading at a given strain produces less plastic strain than that resulting from a longer duration of loading at the same strain. This behavior is consistent with three types of displacement histories used to monitor the plastic strain response.; The stress behavior differs markedly from that expected for a linear viscoelastic material. We see that the stress developed is much lower than predicted for a viscoelastic material based on the infinitesimal strain frequency sweep, and the rate of relaxation of stress is more rapid than for that material. During quasi-static loading the stress begins to deviate significantly from linearity with respect to strain at approximately the value of strain where plastic strain is first observed during dynamic loading. This correlation between the deviation from linearity in the stress response and the evolution of plastic strain is not apparent at finite strain rates, where the stress deviates from linearity with respect to stress at a strain higher than that where plastic strain is first observed. Additionally, the stress response returns to linearity with respect to the difference between the strain and the plastic strain when the material is unloaded from a viscoelastic-plastic state.; When a small oscillatory strain is superimposed on a step strain the phase angle exhibits a nonlinear transient response. At long times both the plastic strain rate and the rate of decrease of the phase angle approach zero. Thus, at long time the material again appears to behave as a linear viscoelastic material.; We have developed a model to describe the viscoplastic response and the stress response, and the model has been used to predict the amount of plastic strain developed after several types of strain histories. Our model has been able to predict the qualitative behavior of the observed plastic strain response as a function of time and strain for applied strain experiments, and as a function of stress and time for the case of step stress. In predicting the stress response, the model was able to account for the qualitative trend of the phase angle with respect to time and frequency and the behavior of the phase angle as the strain is increased. In most cases the predicted values of the phase angle were far too low. Additionally, our attempt to predict the stress in other strain histories met with limited success. (Abstract shortened by UMI.)
机译:我们已经在有限应变下进行了一系列实验,这些实验表明液晶共聚酯Vectra具有一个粘弹性行为区域,在该区域中所有应变都可以恢复,并且应力响应近似线性。我们还发现,在该区域之外的应变处,聚合物以非线性粘弹性材料的形式响应,并且并非所有应变都可恢复。我们试图构建一个简单的模型来描述这种行为。在应变为0.005或更大时,该材料显然表现为非线性粘弹性-粘塑性材料。此行为最容易看到的方面是不可恢复应变的发展及其对应变历史的依赖性。塑性应变是所施加应变的函数。而且,与在相同应变下较长的加载持续时间相比,在给定应变下较短的持续加载产生的塑性应变较小。这种行为与用于监测塑性应变响应的三种位移历史一致。应力行为与线性粘弹性材料的预期行为明显不同。我们看到,根据无限微小的应变频率扫描,所产生的应力远低于粘弹性材料的预测值,并且应力的松弛速率比该材料要快。在准静态载荷过程中,应力相对于应变开始显着偏离线性,近似于动态载荷过程中首次观察到塑性应变的应变值。在有限应变速率下,应力响应中的线性偏差与塑性应变演变之间的这种相关性并不明显,在有限应变率下,应力相对于应力的线性偏离性高于首次观察到塑性应变的线性应变。另外,当从粘弹塑性状态卸载材料时,应力响应相对于应变和塑性应变之间的差异恢复线性。当在阶跃应变上叠加一个小的振荡应变时,相角会表现出非线性瞬态响应。在长时间内,塑性应变率和相角的减小率都接近零。因此,在很长一段时间内,该材料再次表现为线性粘弹性材料。我们已经开发了描述粘塑性响应和应力响应的模型,并且该模型已被用于预测在几种类型的应变历史之后产生的塑性应变的量。我们的模型已经能够预测所观察到的塑性应变响应的定性行为,对于所应用的应变实验,该响应是时间和应变的函数,对于阶跃应力,则是应力和时间的函数。在预测应力响应时,该模型能够说明相角相对于时间和频率的定性趋势,以及随着应变增加而发生的相角行为。在大多数情况下,相角的预测值太低。此外,我们尝试预测其他应变历史中的应力的尝试取得了有限的成功。 (摘要由UMI缩短。)

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