Electric field criteria for charge packet formation and movement in XLPE

The formation of space charge packets in crosslinked polyethylene (XLPE) tapes from un-aged cable insulation has been studied utilizing the pulsed electroacoustic (PEA) technique. The 150 /spl mu/m thick sheets were studied under constant applied DC field of 120 kV/mm at a temperature of 20/spl deg/C for a period of 48 h. After an inception period of /spl sim/3.5 h, during which heterocharge accumulates at the anode and increases the local field there, a sequence of positive charge packets was observed to transit the sample starting from near the anode. Calculation of the internal field showed that the packets required a field of /spl ges/140 kV/mm for their initiation. Reduction of the applied field step-wise from 120 to 80 kV/mm indicated that the charge packet would keep moving as long as the local field at its front was >100 kv/mm, but with a reducing magnitude. A return to an applied field of 120 kV/mm confirmed that the local field required to initiate a new packet was >135 kV/mm. The results are discussed in terms of current theories of charge packet formation. The first packet appears to be a moving front of field ionization. The generation of subsequent packets is governed by the field at the anode and the balance of charge injection and extraction process, which occur there. The nature of the negative charges produced at the ionization front is not clear, but they are unlikely to be electrons.

[1]  Bruce S. Bernstein,et al.  Recent progress in understanding water treeing phenomena , 1984, 1984 IEEE International Conference on Eletrical Insulation.

[2]  A. See,et al.  Space charge and associated electroluminescence processes in XLPE cable peelings , 2000, 2000 Annual Report Conference on Electrical Insulation and Dielectric Phenomena (Cat. No.00CH37132).

[3]  D. Mary,et al.  A note on charge recombination in low density polyethylene under a moderate ac 50 Hz field , 2000 .

[4]  T. Okamoto,et al.  Space charge behavior in XLPE cable insulation under 0.2-1.2 MV/cm dc fields , 1998 .

[5]  A. See,et al.  Advanced pulsed electro-acoustic system for space charge measurement , 2000 .

[6]  T. Okamoto,et al.  Direct observation of time-dependent space charge profiles in XLPE cable under high electric fields , 1994 .

[7]  T. Takada,et al.  Observation of charge behavior in organic photoconductor using pressure wave propagation method , 1991, [1991] Proceedings of the 3rd International Conference on Properties and Applications of Dielectric Materials.

[8]  A. See,et al.  Characterizing HV XLPE cables by electrical, chemical and microstructural measurements on cable peeling: effects of surface roughness, thermal treatment and peeling location , 2000, 2000 Annual Report Conference on Electrical Insulation and Dielectric Phenomena (Cat. No.00CH37132).

[9]  T. Takada,et al.  Pulsed electro-acoustic method for measurement of space charge distribution in power cables under both DC and AC electric fields , 1993 .

[10]  Y. Suzuoki,et al.  Computer simulation on formation of space charge packets in XLPE films , 1999 .

[11]  JULIAN F. Johnson,et al.  Analysis of antioxidants in polymers by liquid chromatography , 1980 .

[12]  A. Cherifi,et al.  The validation of the thermal step method , 1992 .

[13]  Tatsuo Takada Acoustic and optical methods for measuring electric charge distributions in dielectrics , 1999 .

[14]  M. Ieda,et al.  Packet-like space charges and conduction current in polyethylene cable insulation , 1996 .

[15]  Julia Alison,et al.  A high field pulsed electro-acoustic apparatus for space charge and external circuit current measurement within solid insulators , 1998 .