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1.
热塑性聚合物经受稳定的银纹微纤拉伸时,银纹区的迅速增厚将会迅速地引起局部绝热升温现象.预测裂尖银纹的热力学分析可以预测结晶热塑性高聚物冲击断裂阻抗.热反内聚模型用来模拟冲击拉伸过程银纹寿命或反内聚时间.文中报道了一种新型的全切痕蠕变测试法可以在银纹增厚速率高达2m/s时测量平面银纹层的内聚力,在快速拉伸条件下高密度聚乙烯的内聚力和银纹寿命被测量,测试的结果与数值模型的预测结果是相一致的. 相似文献
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高聚物银纹断裂的研究现状 总被引:6,自引:0,他引:6
银纹化是高聚物的一种非线性变形方式,对高聚物的增韧设计十分重要。考虑银纹细观结构特征的银纹生长和断裂规律是研究银纹增韧机制的核心内容。结合国内外最新的研究进展,对承载高聚物中的银纹断裂及其与裂纹扩展的相互作用等问题作了较全面的总结和分析,并对今后的研究重点和趋势作了简要展望。 相似文献
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Although CO2 at 1 atmosphere pressure is not a crazing and/or cracking agent for polystyrene (PS), we have established that it becomes one at higher pressure. Crazes grown from cracks in PS thin films in high pressure CO2 are investigated using transmission electron microscopy (TEM). The fact that broken craze fibrils retract strongly upon exposure to high pressure CO2 gas suggests that the primary effect of the CO2 is plasticization, not surface energy reduction. Quantitative analyses of TEM micrographs of crazes grown at CO2 pressures in the range 5 to 100 MPa at 34°C and 45°C have been carried out to find the craze fibril volume fractions vf(x) and the surface displacements w(x) along each craze. From the fibril volume fraction profile along the craze, the dominant craze thickening mechanism of CO2 crazes is shown to be the same as that for air crazes, i.e. the surface drawing mechanism, and not the fibril creep mechanism. The craze surface stress profile is computed from the craze surface displacements using a distributed dislocation analysis. These profiles all show a stress concentration at the craze tip which falls to a roughly constant value σb, over the rest of the craze. The fracture toughness GIc (and critical stress intensity factor KIc) for propagation of a crack in PS at these CO2 pressures can also be computed. All these quantities (Vf, σb, GIc and KIc) show pronounced minima as a function of CO2 pressure at 20 MPa, the same CO2 pressure at which Tg of the polymer also reaches a minimum. These minima are more pronounced at 45°C than at 34°C. The GIc's and KIc's are depressed by orders of magnitude at the minimum, which corresponds to the qualitative observation that CO2 becomes a severe cracking agent at these pressures. These observations provide additional confirmation that the major mechanism for the environmental crazing and cracking of PS by CO2 is plasticization of the craze fibrils and surfaces. 相似文献
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Crazes formed under a constant tensile strain in polystyrene (PS) have a dense network of fibrils with an extension ratio , but a midrib of higher λ forms by drawing fibrils from the craze-matrix interface in the high stress region just behind the craze tip. Stepwise increases in tensile strain during craze growth should thus produce layers of fibrils of different λ, which can be revealed by transmission electron microscopy (TEM) of crazes in stepwise strained PS films. When the time interval between strain increments of 0.5–1% is one minute, TEM images show ‘ridges’ of lower λ fibrils, corresponding to the position of the craze-matrix interface at the time of the strain increments. The ridges appear to be the analogue of the bulge remaining on a macroscopic fibre which has been allowed to stress age by stress relaxation before resuming drawing and imply that rapid stress ageing must occur near rthe craze-matrix interface so that more material is drawn into the craze in preference to increasing the λ of the existing fibrils. 相似文献
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