Effect of reverse polarity on space charge evolution in polypropylene with different concentration of natural and synthetic nano clay

M. Abou-Dakka, Yaoren Chen
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引用次数: 9

Abstract

Space charge evolution in Polypropylene (PP) loaded with two types of nanoparticles, synthetic and natural clay were investigated using weekly reversing polarity. The space charges were measured with the PEA technique after certain periods of poling with both polarities. The charge distribution in the host materials was substantially smaller with reverse polarity compared to single negative polarity. This majority of charge injected with single polarity is likely due to compatibilizers, which are polar materials. The apparent charges due to dipoles are neutralized when the field is inversed and the remaining charges that fall in deep traps require more than ± 25 kV/mm to be released. To obtain and maintain space charge suppression for both polarities the nanoclay concentration in PP should be below the percolation threshold and ensure uniform distribution of nano-particles throughout polymer matrix. The PNC with 2-wt% of synthetic clay stores lots of charges with reverse polarity, especially after the end of the positive periods. So the synthetic PNC with 2-wt% will not be an optimal concentration. It is seen that 4-wt% (PP1-S4%) for the synthetic PNC and the 2-wt% (PP2-N2%) for the natural PNC are the optimal PNC concentrations. They store minimal charge, particularly in central zones. The absolute value of charge with reverse polarity of all the filled and unfilled materials could store charges relatively of same order. The quantity of charge in the unfilled material, PP1-0% shows continuous increase of charges and it becomes higher than the filled PNC, (except the PP1-S2%), after the 1st W of single polarity poling and the 12th W of reverse polarity poling. But the quantity of charge in the natural PNC was small and unaffected by the loading with nanoclay. Therefore, more poling time is necessary to examine the effect of long term poling on the charge evolution as we have reported earlier for single poling.
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反极性对天然和合成纳米粘土不同浓度聚丙烯中空间电荷演化的影响
采用周极性反转方法研究了合成纳米粒子和天然纳米粒子在聚丙烯(PP)中的空间电荷演化。在两个极性极化一定时间后,用PEA技术测量了空间电荷。与单负极性相比,反向极性下宿主材料中的电荷分布要小得多。这种以单极性注入的大部分电荷可能是由于相容剂,这是极性材料。偶极子产生的视电荷在电场反转时被中和,剩余的落入深阱的电荷需要超过±25 kV/mm才能释放。为了获得并维持两极性的空间电荷抑制,PP中的纳米粘土浓度必须低于渗透阈值,并保证纳米颗粒在聚合物基体中的均匀分布。含2 wt%合成粘土的PNC储存了大量极性相反的电荷,特别是在正极期结束后。因此,2 wt%的合成PNC不是最佳浓度。可以看出,合成PNC的4-wt% (PP1-S4%)和天然PNC的2-wt% (PP2-N2%)是最佳的PNC浓度。它们储存的电量很少,尤其是在中心区域。所有填充和未填充材料的极性相反的电荷绝对值可以存储相对相同的顺序的电荷。在单极性极化第1 W和反极性极化第12 W后,未填充材料PP1-0%的电荷量呈现出持续增加的趋势,并高于填充后的PNC (pp1 - 2%除外)。但天然PNC的电荷量很小,且不受纳米粘土加载的影响。因此,我们需要更多的极化时间来研究长期极化对电荷演变的影响,正如我们之前报道的那样。
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