Experimental Determination of the Current Constriction Characteristics at the Anode of AMF Vacuum Arcs
Before the formation of the anode spot, the anode current constriction is considered as a result of current constriction on the cathode surface and in the arc column. The objective of this paper is to quantitatively determine the current constriction characteristics by experiments at the anode of va...
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Published in | IEEE transactions on plasma science Vol. 47; no. 9; pp. 4361 - 4369 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
New York
IEEE
01.09.2019
The Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
Subjects | |
Online Access | Get full text |
ISSN | 0093-3813 1939-9375 |
DOI | 10.1109/TPS.2019.2930297 |
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Abstract | Before the formation of the anode spot, the anode current constriction is considered as a result of current constriction on the cathode surface and in the arc column. The objective of this paper is to quantitatively determine the current constriction characteristics by experiments at the anode of vacuum arcs under an axial magnetic field (AMF). In this paper, the radial distribution of the anode current density in a diffused vacuum arc was determined quantitatively by a novel method of four types of split-anode contacts, with various diameters of the central areas. The vacuum arc was in the diffuse arc mode with the arc current ranging from 6-to 14-kA rms. An external AMF was applied at 74 mT. The results indicate that the radial distribution of the anode current density <inline-formula> <tex-math notation="LaTeX">j_{z} </tex-math></inline-formula> is in the form of the three-parameter equation, <inline-formula> <tex-math notation="LaTeX">j_{z}=aj_{A}e^{(-br\wedge 2)}+c </tex-math></inline-formula>, where <inline-formula> <tex-math notation="LaTeX">j_{A} </tex-math></inline-formula> is the average current density on the whole anode surface, <inline-formula> <tex-math notation="LaTeX">r </tex-math></inline-formula> is the radius of the anode contact, and the value of constants <inline-formula> <tex-math notation="LaTeX">a </tex-math></inline-formula>, <inline-formula> <tex-math notation="LaTeX">b </tex-math></inline-formula>, and <inline-formula> <tex-math notation="LaTeX">c </tex-math></inline-formula> depends on the arc current. Moreover, the results reveal the constriction characteristics of the anode current density in high-current vacuum arcs subject to the AMF, which was quite uneven in the radial distribution of the anode current density in the diffuse arc mode. Finally, under various arc currents, the constriction characteristics of the anode current density reveal similar patterns. The current density mainly constricted in the central region, in which the diameter might be only one-third of the whole diameter of the anode contact. |
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AbstractList | Before the formation of the anode spot, the anode current constriction is considered as a result of current constriction on the cathode surface and in the arc column. The objective of this paper is to quantitatively determine the current constriction characteristics by experiments at the anode of vacuum arcs under an axial magnetic field (AMF). In this paper, the radial distribution of the anode current density in a diffused vacuum arc was determined quantitatively by a novel method of four types of split-anode contacts, with various diameters of the central areas. The vacuum arc was in the diffuse arc mode with the arc current ranging from 6-to 14-kA rms. An external AMF was applied at 74 mT. The results indicate that the radial distribution of the anode current density [Formula Omitted] is in the form of the three-parameter equation, [Formula Omitted], where [Formula Omitted] is the average current density on the whole anode surface, [Formula Omitted] is the radius of the anode contact, and the value of constants [Formula Omitted], [Formula Omitted], and [Formula Omitted] depends on the arc current. Moreover, the results reveal the constriction characteristics of the anode current density in high-current vacuum arcs subject to the AMF, which was quite uneven in the radial distribution of the anode current density in the diffuse arc mode. Finally, under various arc currents, the constriction characteristics of the anode current density reveal similar patterns. The current density mainly constricted in the central region, in which the diameter might be only one-third of the whole diameter of the anode contact. Before the formation of the anode spot, the anode current constriction is considered as a result of current constriction on the cathode surface and in the arc column. The objective of this paper is to quantitatively determine the current constriction characteristics by experiments at the anode of vacuum arcs under an axial magnetic field (AMF). In this paper, the radial distribution of the anode current density in a diffused vacuum arc was determined quantitatively by a novel method of four types of split-anode contacts, with various diameters of the central areas. The vacuum arc was in the diffuse arc mode with the arc current ranging from 6-to 14-kA rms. An external AMF was applied at 74 mT. The results indicate that the radial distribution of the anode current density <inline-formula> <tex-math notation="LaTeX">j_{z} </tex-math></inline-formula> is in the form of the three-parameter equation, <inline-formula> <tex-math notation="LaTeX">j_{z}=aj_{A}e^{(-br\wedge 2)}+c </tex-math></inline-formula>, where <inline-formula> <tex-math notation="LaTeX">j_{A} </tex-math></inline-formula> is the average current density on the whole anode surface, <inline-formula> <tex-math notation="LaTeX">r </tex-math></inline-formula> is the radius of the anode contact, and the value of constants <inline-formula> <tex-math notation="LaTeX">a </tex-math></inline-formula>, <inline-formula> <tex-math notation="LaTeX">b </tex-math></inline-formula>, and <inline-formula> <tex-math notation="LaTeX">c </tex-math></inline-formula> depends on the arc current. Moreover, the results reveal the constriction characteristics of the anode current density in high-current vacuum arcs subject to the AMF, which was quite uneven in the radial distribution of the anode current density in the diffuse arc mode. Finally, under various arc currents, the constriction characteristics of the anode current density reveal similar patterns. The current density mainly constricted in the central region, in which the diameter might be only one-third of the whole diameter of the anode contact. |
Author | Geng, Yingsan Xiao, Xiangwen Wang, Jianhua Ma, Hui Liu, Zhiyuan Zhang, Zaiqin |
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SubjectTerms | Anodes Axial magnetic field (AMF) Cathodes Constrictions Current density Current distribution Electric arcs Magnetic fields Plasma Plasmas Radial distribution vacuum arc Vacuum arcs |
Title | Experimental Determination of the Current Constriction Characteristics at the Anode of AMF Vacuum Arcs |
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