首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >SPACE CHARGE DISTRIBUTION IN LOW-DENSITY POLYETHYLENE WITH CHARGE-INJECTION SUPPRESSION LAYERS
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SPACE CHARGE DISTRIBUTION IN LOW-DENSITY POLYETHYLENE WITH CHARGE-INJECTION SUPPRESSION LAYERS

机译:带电荷注入层的低密度聚乙烯中的空间电荷分布

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Space charges formed in low-density polyethylene (LDPE), to which high voltage is applied, are usually composed of injected homocharges from electrodes and ionized heterocharges from bulk impurities. In this paper, the heterocharges in LDPE were discriminated from homocharges using charge-injection suppression layers. Recent advanced techniques have made it possible to observe directly the space charge distributed in dielectrics. However, it is difficult to study the characteristics of charge injection from electrodes and ionization of impurities individually as the two processes may interfere with each other and become inseparable. Therefore, a layer that suppresses the charge injection from electrodes was used to discriminate between injected and ionized charges. To observe the space-charge distributions, the pulsed electroacoustic (PEA) method, one of the advanced techniques, was employed. In LDPE with suppression layers on both surfaces, hetero-space charges, which are attributed to ionization of impurities, were observed. On the other hand, in LDPE without the suppression layers, small amounts of home-space charges, which are attributed to net charges from both the electrode injection and the bulk ionization, were observed. Amounts of charge supplied from electrodes were estimated by subtracting the amount of space charge in the sample with suppression layers from that in the sample without suppression layers. [References: 13]
机译:在低密度聚乙烯(LDPE)上施加的高压所形成的空间电荷通常由电极注入的均电荷和体相杂质的离子化电荷组成。在本文中,使用电荷注入抑制层将LDPE中的杂电荷与均电荷区分开。最近的先进技术使直接观察分布在电介质中的空间电荷成为可能。然而,由于两个过程可能相互干扰并且变得不可分割,因此难以分别研究从电极注入的电荷和杂质的电离的特性。因此,使用抑制来自电极的电荷注入的层来区分注入的电荷和电离的电荷。为了观察空间电荷分布,采用了一种先进的脉冲电声(PEA)方法。在两个表面均具有抑制层的LDPE中,观察到归因于杂质电离的异空间电荷。另一方面,在不具有抑制层的LDPE中,观察到少量归属空间电荷,该归属空间电荷归因于来自电极注入和本体电离的净电荷。通过从不具有抑制层的样品中减去具有抑制层的样品中的空间电荷量,可以估算出从电极提供的电荷量。 [参考:13]

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