Early stages of negative PD development in dielectric liquids

The pulse shapes in the early stages of partial discharge (PD) development, well before liquid streamer onset, and obtained with a 500 MHz wide band detection system using needle-to-metallic plane electrodes submerged in a mineral oil, were compared to those measured with needle to mineral oil plane electrodes in air under negative dc potential. All measurements were carried out /spl ap/50% below the breakdown field value, using gap separations between 3 and 25 mm. Whereas the needle to plane discharge behavior in the mineral oil was characterised by discrete sporadic pulses or burst of several pulses of increasing negative amplitude and oscillatory form, the needle to mineral oil plane gap in air gave rise to primarily dense bursts of unidirectional negative pulses with sequentially decreasing amplitude. The pulses had rise times typically of the order of 1 to 2 ns, indicating the involvement of rapid PD mechanisms. >

[1]  R. Bartnikas,et al.  Ionization and excitation behavior in a microcavity , 1995 .

[2]  Olivier Lesaint,et al.  Initiation and propagation thresholds of positive prebreakdown phenomena in hydrocarbon liquids , 1994 .

[3]  Ultrahigh frequency study of PD pulses , 1994, Proceedings of 1994 IEEE International Symposium on Electrical Insulation.

[4]  R. Bartnikas,et al.  Multiple stress aging of solid-dielectric extruded dry-cured insulation systems for power transmission cables , 1994 .

[5]  Massimo Pompili,et al.  The effect of the definition used in measuring partial discharge inception voltages , 1993 .

[6]  E. O. Forster,et al.  Partial discharges and streamers in liquid dielectrics-the significance of the inception voltage , 1993 .

[7]  Massimo Pompili,et al.  A comparison of streamer and partial discharge inception voltages in liquid dielectrics , 1992 .

[8]  Massimo Pompili,et al.  Partial discharge distributions in liquid dielectrics , 1992 .

[9]  J. P. Steiner,et al.  Recent advances in partial discharge measurement capabilities at NIST , 1992 .

[10]  H. G. Sedding,et al.  Practical implementation of ultrawideband partial discharge detectors , 1992 .

[11]  C. Mazzetti,et al.  The effect of molecular structure on the properties of dielectric fluids , 1991 .

[12]  W. G. Chadband,et al.  The role of electrostatic and hydrodynamic forces in the negative-point breakdown of liquid dielectrics , 1991 .

[13]  S. V. Kulkarni,et al.  Influence of a dielectric barrier on the stochastic behaviour of Trichel-pulse corona , 1991 .

[14]  E. Forster,et al.  Progress in the understanding of electrical breakdown in condensed matter , 1990 .

[15]  Kulkarni,et al.  Stochastic properties of Trichel-pulse corona: A non-Markovian random point process. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[16]  O. Lesaint,et al.  Investigations on transient currents associated with streamer propagation in dielectric liquids , 1990, 10th International Conference on Conduction and Breakdown in Dielectric Liquids.

[17]  T. V. Blalock,et al.  Observations of partial discharges in hexane under high magnification , 1990, 10th International Conference on Conduction and Breakdown in Dielectric Liquids.

[18]  T. Kaneda,et al.  First Negative Corona Pulses in 70% N2+30%SF6 Mixture , 1989 .

[19]  T. V. Blalock,et al.  Low-noise wide-band amplification system for acquiring prebreakdown current pulses in liquid dielectrics , 1989 .

[20]  T. V. Blalock,et al.  Prebreakdown current pulses in n-hexane and other dielectric fluids , 1989 .

[21]  T. V. Blalock,et al.  Measurement of partial discharges in hexane under DC voltage , 1988, 1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena.

[22]  W. G. Chadband,et al.  The dynamics of pre-breakdown cavities in viscous silicone fluids in negative point-plane gaps , 1988 .

[23]  Massimo Pompili,et al.  A comparative evaluation of partial discharge inception voltage of power transformer liquids , 1988, Conference Record of the 1988 IEEE International Symposium on Electrical Insulation.

[24]  R. Hebner,et al.  Simultaneous measurement of light emission, current pulses and growth of prebreakdown streamers in hexane , 1987, Conference on Electrical Insulation & Dielectric Phenomena — Annual Report 1987.

[25]  G. Haddad,et al.  Negative corona in nitrogen−oxygen mixtures , 1987 .

[26]  O. Lesaint,et al.  Streamer generation and propagation in transformer oil under divergent field conditions , 1987, 1987 Ninth International Conference on Conduction and Breakdown in Dielectric Liquids.

[27]  H. I. Marsden,et al.  DC-Induced Prebreakdown Events in N-Hexane , 1986, IEEE Transactions on Electrical Insulation.

[28]  Morrow Theory of stepped pulses in negative corona discharges. , 1985, Physical review. A, General physics.

[29]  T. J. Lewis,et al.  The 1984 H. Tropper Memorial Lecture Electronic Ppocesses in Dielectric Liquids Under Incipient Breakdown Stress , 1985, IEEE Transactions on Electrical Insulation.

[30]  H. Yamashita,et al.  Pre-Breakdown Current and Light Emission in Transformer Oil , 1984, IEEE Transactions on Electrical Insulation.

[31]  S.A. Boggs,et al.  Wide band measurements of partial discharge in epoxy , 1982, 1982 IEEE International Conference on Electrical Insulation.

[32]  Richard J. Van Brunt,et al.  Characterization of point‐plane corona pulses in SF6 , 1981 .

[33]  P. Watson EHD instabilities in the breakdown of point-plane gaps in insulating liquids , 1981, Conference on Electrical Insulation & Dielectric Phenomena - Annual Report 1981.

[34]  J. C. Devins,et al.  Breakdown and prebreakdown phenomena in liquids , 1981 .

[35]  J. K. Nelson,et al.  A divergent field study of prebreakdown events in n-hexane , 1979 .

[36]  T. Ishii,et al.  Partial Discharge Characteristics of Silicone Liquids , 1976, IEEE Transactions on Electrical Insulation.

[37]  W. R. L. Thomas,et al.  An ultra-high speed laser schlieren technique for studying electrical breakdown in dielectric liquids , 1973 .

[38]  Z. Krasucki,et al.  Breakdown of liquid dielectrics , 1966, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[39]  B Farazmand,et al.  Study of electric breakdown of liquid dielectrics using Schlieren optical techniques , 1961 .

[40]  A. Harry Sharbaugh,et al.  High‐Field Conduction Currents in Liquid n‐Hexane under Microsecond Pulse Conditions , 1960 .

[41]  T. Lewis Electric Strength and Liquid Structure , 1957 .

[42]  T. J. Lewis,et al.  Mechanism of Electrical Breakdown in Saturated Hydrocarbon Liquids , 1956 .

[43]  J. Bragg,et al.  Dependence of the Electric Strengths of Liquids on Electrode Spacing , 1955 .

[44]  M. R. Amin Fast Time Analysis of Intermittent Point‐to‐Plane Corona in Air. III. The Negative Point Trichel Pulse Corona , 1954 .

[45]  L. Loeb,et al.  Recent Developments in Analysis of the Mechanisms of Positive and Negative Coronas in Air , 1948 .

[46]  G. W. Trichel The Mechanism of the Positive Point-to-Plane Corona in Air at Atmospheric Pressure , 1939 .