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Effects of LDPE/nanofilled LDPE interface on space charge formation

机译:LDPE /纳米填充LDPE界面对空间电荷形成的影响

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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 wi- l be helpful for further optimization of HVDC cable.
机译:双层电介质,它由低密度聚乙烯(LDPE)和纳米二氧化钛填充LDPE(命名的TiO 2 -LDPE)的空间电荷特性,已通过脉冲电声(PEA)方法测试下不同高压直流(HVDC)的电场。在TiO 2 -LDPE材料通过掺杂纳米的TiO 2 成具有0.5每百份份树脂(phr)的重量不同比例的无添加剂的LDPE,2份制造和5份,分别。此外,在空间电荷行为LDPE /二氧化钛 2 -LDPE界面的影响进行了讨论,当LDPE层是无论在阳极和阴极侧通过反转双层电介质。结果表明,正载流子积聚在样品的其LDPE层位于阳极侧时电场增大到一定值的接口。然而,负载流子积累发生在样品的其LDPE层在阴极侧的界面。的电场越高,积累的界面电荷的量越大。但有电荷量具有不同的纳米氧化钛 2 浓度系统之间无明显差异。界面空间电荷的形成被认为是LDPE和TiO之间的导电性差,结果 2 -LDPE以及表面形貌的影响。此外,可以看出,当LDPE层是在阳极侧在阴极电荷峰变宽。与此同时,当LDPE层是在阴极的侧面上的小的正电荷峰出现邻近阴极和阳极处变宽电荷峰。目前,此案正在5份最明显。它被认为是由的界面电荷感应电荷引起的。感应电荷具有相反的极性和分发电极附近。结果提供了一种有效的空间电荷控制方法,该方法使得有可能以定位所要求的位置的空间电荷。它的Wi-l条高压直流输电电缆的进一步优化有益的。

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