TY - JOUR
T1 - Inverse calculation of surface charge based on surface potential measurement
AU - Fu, Yangyang
AU - Wang, Qiang
AU - Zhang, Guixin
AU - Wang, Xinxin
PY - 2013/1
Y1 - 2013/1
N2 - Distribution of surface charge can not be directly measured with current techniques but only be determined by complicate inverse calculations based on the results from indirect measurements. Therefore, we studied methods for the inverse calculation, and presented an improved method on the basis of the method proposed by Ootera and his colleagues. In the improved method, the original twice inverses of the incidence matrix were simplified to a once inverse. The surface charge accumulated on cone-type insulator in the air or the SF6 gas under DC voltage was calculated using the improved method. The results show that the distribution of the surface free charge obtained with the improved method is the same as that with the unimproved method. Compared with the original algorithm, the improved method can further obtain the density distributions of surface apparent charge and polarization charge. Moreover, it is found that, in the same gas environment, there is a significant difference in the amplitude of surface density between free charge and apparent charge, which is 370 and 530 pC/cm2 in the air and SF6 gas, respectively.
AB - Distribution of surface charge can not be directly measured with current techniques but only be determined by complicate inverse calculations based on the results from indirect measurements. Therefore, we studied methods for the inverse calculation, and presented an improved method on the basis of the method proposed by Ootera and his colleagues. In the improved method, the original twice inverses of the incidence matrix were simplified to a once inverse. The surface charge accumulated on cone-type insulator in the air or the SF6 gas under DC voltage was calculated using the improved method. The results show that the distribution of the surface free charge obtained with the improved method is the same as that with the unimproved method. Compared with the original algorithm, the improved method can further obtain the density distributions of surface apparent charge and polarization charge. Moreover, it is found that, in the same gas environment, there is a significant difference in the amplitude of surface density between free charge and apparent charge, which is 370 and 530 pC/cm2 in the air and SF6 gas, respectively.
KW - Cone-type insulator
KW - Electrostatic probe
KW - Surface charge of insulator
KW - Surface flashover
KW - Surface potential of insulator
KW - Vibrating Kelvin probe
UR - http://www.scopus.com/inward/record.url?scp=84874389326&partnerID=8YFLogxK
U2 - 10.3969/j.issn.1003-6520.2013.01.013
DO - 10.3969/j.issn.1003-6520.2013.01.013
M3 - Article
AN - SCOPUS:84874389326
SN - 1003-6520
VL - 39
SP - 88
EP - 95
JO - Gaodianya Jishu/High Voltage Engineering
JF - Gaodianya Jishu/High Voltage Engineering
IS - 1
ER -