橡胶的应变诱导结晶及力学性能。: 3。静态和动态条件下的应变诱导结晶

S. Toki
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引用次数: 0

摘要

在静态和动态条件下研究了橡胶的应变致晶化过程。静态条件是指试样保持在一定的应变,动态条件是指试样以一定的速度被拉伸。应考虑两种情况的差异。1.在静态条件下,降低温度可显著降低应力,提高SIC晶率。应力随温度线性降低。应力减小倾斜度大于T/T0(T:绝对温度,T0:参考绝对温度)。T/T0的倾角表示温度的降低导致微布朗运动的减弱。因此,倾角越大,表明网络密度也随着温度的降低而降低。SIC晶率随温度的降低呈线性增加。因此,SIC晶体的形成减少了非晶链的数量。2. 在静态条件下,温度升高使应力增大,SIC晶率降低。应力随温度升高而线性增加。应力增加的倾角为T/T0。这意味着微布朗运动随温度升高而增加,但网络密度不随SIC晶分数的降低而变化。在80℃以上,应力最大,随温度升高而减小。由于SIC晶分数随温度升高而线性降低,应力行为与SIC无直接关系。3.在动态条件下,未硫化的IR在25°C以上不表现SIC,但在0°C以下表现SIC。由于未硫化IR是聚合物熔体,SIC接近半结晶塑料的流动诱导结晶(FIC)。未硫化NR在+100°C, +75°C至-25°C, -50°C范围内具有SIC性能。SIC的起始应变随温度升高而增大。4. 在动态条件下,未硫化NR和硫化NR在-50℃~ +100℃范围内均表现出SIC的性能。SIC的起始应变随温度升高而增大(-50℃除外)。大应变下的应力随温度升高而减小,但应力的减小似乎并不简单,因为从-25°C到+25°C和从+25°C到+100°C的应力减小的倾斜度有显著差异。应力和抗拉强度似乎与SIC没有直接关系。5. 网络密度和网络结构不改变SIC的起始应变。未硫化NR的SIC的起始应变小于硫化NR的起始应变。因此,橡胶链定向和对准SIC的支点似乎不是一个网络点,而是一个缠结。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Strain-Induced Crystallization and Mechanical Properties of Rubber.: 3.Strain-Induced Crystallization under Static and Dynamic Condition
Strain-induced crystallization(SIC)of rubber has been studied under static and dynamic condition. The static condition means that the sample is kept at a certain strain and the dynamic condition means that the sample is being stretched under certain speed. The difference of both condition should be considered. 1.Under the static condition, lowering temperature decreases stress and increases SIC crystal fraction significantly. The stress decreases linearly with temperature. The inclination of stress decrease is larger than T/T0(T: absolute temperature, T0: reference absolute temperature). The inclination of T/T0 means the decrease of micro-Brownian motion due to the decrease of temperature. Therefore, the larger inclination suggests that the network density also decreases with the lowering of temperature. The SIC crystal fraction increases linearly with lowering temperature. Therefore, the creation of SIC crystal decreases the number of amorphous chains. 2. Under the static condition, elevating temperature increases stress and decreases SIC crystal fraction. The stress increases linearly with elevating temperature. The inclination of stress increase is T/T0. It means that the micro-Brownian motion increases with elevating temperature, but the network density does not change by the decrease of SIC crystal fraction. Beyond 80 °C, the stress shows the maximum and decreases with temperature. Because the SIC crystal fraction decreases with elevating temperature linearly, the stress behavior has no direct relation with SIC. 3. Under the dynamic condition, un-vulcanized IR does not perform SIC beyond 25 °C but does perform SIC below 0 °C. Because un-vulcanized IR is polymer melt, SIC is close to FIC(flow induced crystallization)of semi-crystalline plastics. Un-vulcanized NR perform SIC from +100 °C, +75 °C to -25 °C, -50 °C. The onset strain of SIC increases with temperature. 4. Under the dynamic condition, un-vulcanized NR and vulcanized NR perform SIC at from -50 °C to +100 °C. The onset strain of SIC increases with elevating temperature(except -50 °C). The stress at large strain decreases with elevating temperature, but the decrease of stress does not seem to be simple because the inclinations of the decrease of stress from -25 °C to +25 °C and from +25 °C to +100 °C are significantly different. It seems that the stress and tensile strength do not have direct relation with SIC. 5. Network density and network structure do not change onset strain of SIC. The onset strain of SIC of un-vulcanized NR is smaller than that of vulcanized NR. Therefore, a pivot point to orient and align rubber chains into SIC seems to be not a network point but an entanglement.
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