Influence of impurities on electroconvection in insulating liquids

The concentration of impurities in nonpolar liquids in the test liquids was varied either by removing naturally existing impurities by filtration, or by adding conducting particles of carbon, copper, or iron or insulating particles of alumina to filtered test liquids. It is shown that the measured currents in filtered liquids are influenced by the net change in the concentration of charge carriers due to removal of suspended impurities and charge separation. It is established that small conducting particles (diameters, of 0.07 to 1.4 mu m) have a greater influence on electrohydrodynamic motion than larger particles. Copper particles can reduce the breakdown strength of liquid to a greater extent than from iron particles. Alumina particles did not have any influence on induced liquid motion; however, the dominance of dwell time over transit time, for these particles produced a thin insulating coating on the electrode surface that reduced the current slightly. >

[1]  J. Cross,et al.  The influence of impurities on electrohydrodynamic motion in insulating oils , 1989, Conference on Electrical Insulation and Dielectric Phenomena,.

[2]  Markus Zahn,et al.  Electrohydrodynamic traveling-wave pumping of homogeneous semi-insulating liquids , 1989 .

[3]  J. Cross,et al.  Effects of particulate contamination on electrohydrodynamic motion in insulating liquids , 1989, Proceedings of the 19th Electrical Electronics Insulation Conference,.

[4]  A. Jaksts,et al.  Particulate contamination and stress induced motion in transformer oil , 1987, 1987 Ninth International Conference on Conduction and Breakdown in Dielectric Liquids.

[5]  P. Atten,et al.  The Electrohydrodynamic Origin of Turbulence in Electrostatic Precipitators , 1987, IEEE Transactions on Industry Applications.

[6]  M. Darveniza DEMONSTRATION OF THE EFFECT OF CARBON PARTICLES ON THE AC STRENGTH OF TRANSFORMER OIL. , 1985 .

[7]  J. Gosse,et al.  Electrification of cyclohexane in laminar flow in small-diameter metal pipes , 1984 .

[8]  R. Tobazeon,et al.  Ion injection by metallic electrodes in highly polar liquids of controlled conductivity , 1984, 1984 Eighth International Conference on Conduction and Breakdown in Dielectric Liquids.

[9]  T. Oommen,et al.  Eelectrostatic Charging Tendency of Transformer Oils , 1984, IEEE Transactions on Power Apparatus and Systems.

[10]  M. C. Underwood,et al.  An investigation into the conductivity of hydrocarbon liquids , 1984 .

[11]  C. Murphy Handbook of Particle Sampling and Analysis Methods , 1984 .

[12]  T. Oommen,et al.  Particle Contamination Levels in Oil-Filled Large Power Transformers , 1983, IEEE Transactions on Power Apparatus and Systems.

[13]  J. Cross Breakdown Across a Dielectric Spacer in Insulating Oil and the Role of Electrohydrodynamics in Liquid Breakdown , 1982, IEEE Transactions on Electrical Insulation.

[14]  Kamal Miners,et al.  Particles and Moisture Effect on Dielectric Strength of Transformer Oil Using VDE Electrodes , 1982, IEEE Transactions on Power Apparatus and Systems.

[15]  J. F. Roach,et al.  Liquid and particle motions in transformer oil under 60 Hz stress , 1980, 1980 IEEE International Conference on Electrical Insulation.

[16]  A. Wilson,et al.  Insulating liquids : their uses, manufacture, and properties , 1980 .

[17]  J. Cross,et al.  Electric stress induced motion in transformer oils under 60 Hz stress , 1979 .

[18]  G. Molinari,et al.  Analysis of the charge exchange mechanism between impurities and electrodes in a dielectric liquid , 1979 .

[19]  C. Buffam,et al.  Particles and pulses in n-hexane , 1979 .

[20]  T. J. Gallagher,et al.  Simple Dielectric Liquids: Mobility, Conduction, and Breakdown , 1975 .

[21]  J. Calderwood,et al.  Liquid motion and internal pressure in electrically stressed insulating liquids , 1970 .

[22]  B. Vonnegut,et al.  Enhanced charge transfer in dielectric fluids containing conducting particles , 1967 .