Modelling of supply voltage frequency effect on partial discharge repetition rate and charge amplitude from AC to DC at room temperature

被引:28
|
作者
Seri, P. [1 ]
Naderiallaf, H. [1 ]
Montanari, G. C. [2 ]
机构
[1] Univ Bologna, Dept Elect Elect & Informat Engn DEI, Bologna, Italy
[2] Florida State Univ, CAPS, Tallahassee, FL USA
关键词
Partial discharges; Cavity resonators; Discharges (electric); Mathematical model; Integrated circuit modeling; Firing; Insulation; partial discharge (PD); very low frequency (VLF); power supply frequency; DC voltage supply; polymeric cable insulation; PD repetition rate; PD charge amplitude; INSULATION; IDENTIFICATION; MECHANISM;
D O I
10.1109/TDEI.2019.008552
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
This paper has the purpose to derive an analytical model ("continuum" model) able to describe the behavior of partial discharge (PD) repetition rate and amplitude, occurring in a cavity embedded in polymeric insulation, as a function of the frequency of the supply voltage, going from AC power supply frequency, 50-60 Hz, to DC. In the range between DC and 50-60 Hz focus is made on data coming from tests under AC sinewave with very low frequency (VLF) such as 0.1 Hz and 0.01 Hz, which are commonly used for cable testing. It is shown that the proposed "continuum" model can provide reasonably good fit to the experimental results obtained in the range DC to 60 Hz, regarding PD repetition rate and amplitude. To reach such result, the equivalent circuit is modified from that commonly used and made by fully-capacitive or resistive components, in order to take into account the change of polarization mechanisms which, depending on dielectric material, may play a non-negligible role to establish the repetition rate from low frequency to DC power supply. In addition, the residual voltage after a PD event has to vary with frequency to reach good fitting. Also, it is shown that PD amplitude under DC and VLF can be lower than under AC 50-60 Hz due to the delay time of the firing electron, thus experimental PD amplitude varies with frequency depending on material and defect typology and location.
引用
收藏
页码:764 / 772
页数:9
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