非晶聚合物中裂纹形成与流动和主转变的关系

J.-U. Starke, G. Schulze, G. H. Michler
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引用次数: 12

摘要

在超过TVF (Vogel温度)的蠕变实验中,对聚苯乙烯-丙烯腈(SAN)和聚碳酸酯(PC)的无缺口拉伸棒产生了裂纹并进行了分析。采用小角x射线散射(SAXS)和透射电子显微镜(TEM)研究了裂纹微观结构随温度(T)和载荷(σ)的变化规律。与预期相反,在恒定温度下,最大强度散射矢量(smax)与裂纹原纤维之间的距离成反比,与σ无关。在最高应力(状态III)下,smax与应力无关,原纤维之间的平均距离达到最小值。在中等应力(状态II)下,随着温度的降低,检测到纤维性颤动能量Γ的强烈增加。在TVF附近,Γ达到了聚合物链断裂能的等次值。在最低应力状态下,纤维的形成能量与温度无关,与范德华表面能相对应。纤维形成过程中的分子运动可能与局部应力诱导的聚合物链流动过程(状态I)和α-松弛过程(状态II)有关。不断增加的应力限制了大分子的迁移范围,使其迁移范围越来越短,并且在最高应力下发生了从纤维化裂纹到均匀裂纹的转变或剪切变形过程(状态III)。特别是在负压下。
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Craze formation in amorphous polymers in relation to the flow and main transition

Crazes were produced and analyzed in unnotched tensile bars of poly(styrene-co-acrylonitrile) (SAN) and polycarbonate (PC) in creep experiments above TVF (the Vogel temperature). The craze microstructure was investigated as a function of temperature (T) and load (σ) by means of small angle X-ray scattering (SAXS) and transmission electron microscopy (TEM). Contrary to expectation, the scattering vector of maximum intensity (smax), which is inversely proportional to the distance between the fibrils of crazes, was not linearly dependent on σ at constant temperature. At the highest stresses (regime III), smax was independent of stress, and the average distance between the fibrils reaches a minimum value. At intermediate stresses (regime II), a strong increase of fibrillation energy Γ was detected, as the temperature was reduced. In the vicinity of TVF, Γ reached values of the order of the polymer chain fracture energy. At the lowest stresses (regime I), the energy of fibril formation was independent of temperature and corresponded to the van der Waals surface energy. The molecular motions during fibril formation may be linked to local stress-induced flow processes of polymer chains (regime I) and α-relaxations (regime II). Increasing stress restricts the range of mobility of macromolecules to shorter and shorter units and a transition from the formation of fibrillated crazes to homogeneous crazes or shear deformation processes occurs at the highest stresses (regime III). A pressure—temperature diagram was constructed from the transition between the regimes, particularly at negative pressure.

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