聚合物绝缘系统中的电荷注入和分布

T. Baumann, P. Pfluger, F. Stucki, H. Zeller
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引用次数: 7

摘要

超过临界场强Fc的空间电荷的积累可被视为电树成核和老化的重要机制[1]。对于msec的电压坡道,当超过F = Fc的电压Vc时,空间电荷云会瞬间增长。因此,F永远不会被超过:我们处理场限制空间电荷(参考文献1+2的FLSC模型)。在我们的模型中,Fc的微观物理解释是电荷载流子从非常低的、由陷阱控制的迁移率变为高迁移率的场[1,2]。为了实验验证移动载流子注入的概念,并在场增强点周围形成均匀的空间电荷区,选择了针板几何形状。可以验证FLSC模型的基本思想和定量预测[2,3]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Charge injection and distribution in polymeric insulation systems
The build up of space charge above a critical field strength, Fc, can be regarded as an important mechanism for electrical tree nucleation and ageing [1]. For voltage ramps of msec, a homogeneous space charge cloud grows instantaneously if Vc, the voltage at which F = Fc, is surpassed. As a consequence, F will never be exceeded: we deal with field limiting space charge (FLSC model of ref. 1+2). Within our model, the microscopic physical interpretation of Fc is the field at which charge carriers change from very low, trap-controlled mobility to a high mobility [1,2]. In order to test experimentally the concept of injection of mobile carriers and concomitant formation of a homogeneous space charge zone around a point of field enhancement, a needle-plate geometry was chosen. The basic ideas and the quantitative predictions of the FLSC model could be verified [2,3].
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