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W. Dyke, J. Trolan, E. Martin, J. Barbour (1953)
THE FIELD EMISSION INITIATED VACUUM ARC. I. EXPERIMENTS ON ARC INITIATIONPhysical Review, 91
J. Trump, R. Graaff (1947)
The Insulation of High Voltages in VacuumJournal of Applied Physics, 18
A. Denholm (1958)
The electrical breakdown of small gaps in vacuumCanadian Journal of Physics, 36
L. Atta, R. Graaff, H. Barton (1933)
A New Design for a High-Voltage Discharge TubePhysical Review, 43
L. Cranberg (1952)
The Initiation of Electrical Breakdown in VacuumJournal of Applied Physics, 23
A. Ahearn (1936)
The Effect of Temperature, Degree of Thoriation and Breakdown on Field Currents from Tungsten and Thoriated TungstenPhysical Review, 50
W. Dolan, W. Dyke, J. Trolan (1953)
The field emission initiated vacuum arc. II. The resistively heated emitterVacuum, 4
W. Dyke, J. Trolan (1953)
Field Emission: Large Current Densities, Space Charge, and the Vacuum ArcPhysical Review, 89
J. Chiles (1937)
A Photographic Study of the Vacuum Spark DischargeJournal of Applied Physics, 8
R. Mason (1937)
Breakdown of Vacuum Spark GapsPhysical Review, 52
E. Webster, R. Graaff, J. Trump (1952)
Secondary Electron Emission from Metals under Positive Ion Bombardment in High Extractive FieldsJournal of Applied Physics, 23
W. Boyle, P. Kisliuk, L. Germer (1955)
Electrical Breakdown in High VacuumJournal of Applied Physics, 26
C. Chambers (1934)
Emission of electrons from cold metal surfacesJournal of The Franklin Institute-engineering and Applied Mathematics, 218
SummaryExperiments have been performed in order to get information about the phenomena preceding the electrical breakdown in small vacuum gaps. Most experiments have been made with impulse voltages of different rise times; some complementary results obtained with alternating voltage are also presented. The effect of surface layers on the breakdown voltage and on the pre-breakdown current is discussed. It has been found that the rise time of the voltage affects both the breakdown voltage and the pre-breakdown current. The experiments seem to indicate that breakdown in the underlying circumstances is the result of a discharge in metal vapour, originating from the anode. The vapour is thought to be generated by the heating of the anode by a bombardment of field-emission electrons. The transition of the pre-breakdown current to a sudden discharge may occur when the vapour density passes a critical value.
Applied Scientific Research, Section B – Springer Journals
Published: Feb 1, 1961
Keywords: Rise Time; Breakdown Voltage; Electrical Breakdown; Vapour Density; Breakdown Strength
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