ELECTRICAL AGING OF EXTRUDED DIELECTRIC CABLES - REVIEW OF EXISTING THEORIES AND DATA

Citation
C. Dang et al., ELECTRICAL AGING OF EXTRUDED DIELECTRIC CABLES - REVIEW OF EXISTING THEORIES AND DATA, IEEE transactions on dielectrics and electrical insulation, 3(2), 1996, pp. 237-247
Citations number
50
Categorie Soggetti
Engineering, Eletrical & Electronic
ISSN journal
10709878
Volume
3
Issue
2
Year of publication
1996
Pages
237 - 247
Database
ISI
SICI code
1070-9878(1996)3:2<237:EAOEDC>2.0.ZU;2-B
Abstract
Despite the huge amount of data on so-called electrical aging of extru ded HV cables, the fundamental phenomena responsible for it or evolvin g with aging time, are still far from well understood. It is therefore not surprising why it is so difficult to predict reliable cable lifet imes in service from accelerated aging experiments in the laboratory. The objective of this paper is to review critically the existing theor ies of electrical aging of solid dielectric materials. A relatively la rge number of models and theories exist but none of the most often use d is known to yield reliable life predictions. One conclusion is that there is a need for a more comprehensive model of electrical aging of extruded dielectric cables. In order to develop this model, an extensi ve review of existing literature data was undertaken. This paper summa rizes the data collected from more than 200 papers on aging of PE, XLP E and EPR cables. It appears that cable breakdown strength should not be plotted on log field vs. log time graphs to yield long-time (i.e. l ow-field) values, since results obtained over a long time period do no t obey an inverse power law. In fact, high-field results are better de scribed by an exponential relation between time and field. The models of Simoni, Montanari and Crine seem to give the best fit to experiment al results obtained under a wide variety of experimental conditions. I t is also shown that the lower field limit for the exponential regime with XLPE cable is in the 8 to 15 kV/mm range, which corresponds to th e onset of strong charge injection. The influence of environment, insu lation nature and morphology, and testing temperature are discussed. I t is also shown that the two physical parameters of the model describe d in Part 2 are linearly related and vary with the experimental condit ions.