LDPE/纳米填充LDPE界面对空间电荷形成的影响

N. Zhao, Shengtao Li, Xia Wang, Guochang Li
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引用次数: 7

摘要

采用脉冲电声(PEA)方法对低密度聚乙烯(LDPE)和纳米二氧化钛填充LDPE (TiO2-LDPE)双层介质在不同高压直流(HVDC)电场下的空间电荷特性进行了测试。将纳米tio2掺杂到自由添加剂LDPE中,分别为0.5 /百份树脂(phr)、2 /百份树脂(phr)和5 /百份树脂(phr),制备TiO2-LDPE材料。进一步讨论了LDPE/TiO2-LDPE界面对空间电荷行为的影响,当LDPE层同时位于阳极和阴极两侧时,通过反转双层介质。结果表明,当电场增大到一定值时,LDPE层位于阳极一侧的样品的界面处有正载流子聚集。然而,当LDPE层位于阴极一侧时,样品的界面会发生负载流子积累。电场越大,界面电荷积累量越大。但不同纳米tio2浓度体系的电荷量没有明显差异。界面空间电荷的形成被认为是LDPE与TiO2-LDPE电导率差异以及表面形貌影响的结果。此外,可以看出,当LDPE层位于阳极一侧时,阴极处的电荷峰变宽。同时,在阴极附近出现了一个小的正电荷峰,当LDPE层在阴极一侧时,阳极的电荷峰变宽。这种情况在5小时以下最为明显。它被认为是由界面电荷的诱导电荷引起的。感应电荷具有相反的极性,分布在电极附近。研究结果提供了一种有效的空间电荷控制方法,使空间电荷的定位成为可能。这将有助于进一步优化高压直流电缆。
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Effects of LDPE/nanofilled LDPE interface on space charge formation
Space charge characteristics of double-layer dielectric, which consists of low density polyethylene (LDPE) and nano-titania filled LDPE (named TiO2-LDPE), have been tested by pulsed electro acoustic (PEA) method under different high voltage direct current (HVDC) electric fields. The TiO2-LDPE material is fabricated by doping nano-TiO2 into free additive LDPE with different weight proportions of 0.5 parts per hundred parts of resin (phr), 2 phr and 5 phr, respectively. Furthermore, the effects of LDPE/TiO2-LDPE interface on space charge behavior are discussed when the LDPE layer is both on the side of anode and cathode by reversing the double-layer dielectric. The results indicate that positive carriers accumulate at the interface of samples whose LDPE layer is located on the side of anode when electric field increases to certain value. However, negative carrier accumulation happens to the interface of samples whose LDPE layer is on the side of cathode. The higher the electric field, the larger the amount of interface charges accumulated. But there is no obvious difference of charge amount among systems with different nano-TiO2 concentrations. The formation of the interface space charge is considered as the result of conductivity difference between LDPE and TiO2-LDPE as well as influence of surface morphology. Moreover, it can be seen that the charge peak at cathode broadens when the LDPE layer is on the side of anode. At the same time, a small positive charge peak appears near cathode and the charge peak at anode broadens when the LDPE layer is on the side of cathode. The case is the most obvious under 5 phr. It is believed to be caused by induced charges of the interface charges. The induced charges have opposite polarity and distribute near the electrodes. The results provide an effective space charge controlling method, which makes it possible to locate space charge in the position required. It will be helpful for further optimization of HVDC cable.
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