Space charge accumulation and electric breakdown in XLPE under DC high electric field

Author(s):  
Hitoshi Suzuki ◽  
Ando Nozomu ◽  
Hiroaki Miyake ◽  
Yasuhiro Tanaka ◽  
Takashi Maeno
2005 ◽  
Vol 10 (1) ◽  
pp. 77-82
Author(s):  
F. Kuliešius ◽  
S. Tamošiūnas ◽  
A. Žindulis

The regularities of the dark discharge in ionic contact mode as well as of the thermoelectret effect have been investigated for Zn0.7Cd0.3S layers. The peculiarities of electret charge formation as well as the electret voltage dependences on poling electric field, polarisation time and temperature have been analysed in Zn0.7Cd0.3S layers during the present work. The model of space charge accumulation have been proposed.


2016 ◽  
Vol 198 (3) ◽  
pp. 19-26 ◽  
Author(s):  
TSUYOSHI KATO ◽  
RYO ONOZAWA ◽  
HIROAKI MIYAKE ◽  
YASUHIRO TANAKA ◽  
TATSUO TAKADA

Energies ◽  
2021 ◽  
Vol 14 (5) ◽  
pp. 1313
Author(s):  
Fuqiang Tian ◽  
Shuting Zhang ◽  
Chunyi Hou

Space charge behavior has a strong impact on the long-term operation reliability of high voltage–direct current (HVDC) cables. This study intended to reveal the effect of trap density and depth on the space charge and electric field evolution behavior in HVDC cable insulation under different load currents and voltages by combined numerical bipolar charge transport (BCT) and thermal field simulation. The results show that when the load current is 1800 A (normal value), the temperature difference between the inside and the outside of the insulation is 20 °C, space charge accumulation and electric field distortion become more serious with the increase in the trap depth (Et) from 0.80 to 1.20 eV for the trap densities (Nt) of 10 × 1019 and 80 × 1019 m−3, and become more serious with the increase in Nt from 10 × 1019 to 1000 × 1019 m−3 for Et = 0.94 eV. Simultaneously decreasing trap depth and trap density (such as Et = 0.80 eV, Nt = 10 × 1019 m−3) or increasing trap depth and trap density (such as Et = 1.20 eV, Nt = 1000 × 1019 m−3), space charge accumulation can be effectively suppressed along with capacitive electric field distribution for different load currents (1800 A, 2100 A and 2600 A) and voltages (320 kV and 592 kV). Furthermore, we can draw the conclusion that increasing bulk conduction current by simultaneously decreasing the trap depth and density or decreasing injection current from conductor by regulating the interface electric field via simultaneously increasing the trap depth and density can both effectively suppress space charge accumulations in HVDC cables. Thus, space charge and electric field can be readily regulated by the trap characteristics.


Sign in / Sign up

Export Citation Format

Share Document