The use of vacuum arc discharge as a load for XPG-1 high-current generator

Abstract

It was attempted to use the vacuum arc discharge as a load of a high-current generator. The idea is as follows: metal vapor is injected using the vacuum arc discharge into a microgap of a load unit of the current generator. When the generator current flows over metal vapor, such a load begins to compress as in the classical Z pinch. During compression, Rayleigh-Taylor instabilities develop, which results in the formation of waists and hot spots. The hot spot radiation power can exceed the radiation power in the case of the X pinch used as a load by a factor of 1.5-2. The signal amplitude spread is significantly smaller than that when using the X pinch. The spectrum and sizes of the hot spot can be varied by selecting the mass and type of metal injected into the discharge region.

Original language	English
Pages (from-to)	29-30
Number of pages	2
Journal	Bulletin of the Lebedev Physics Institute
Volume	37
Issue number	1
DOIs	https://doi.org/10.3103/S1068335610010124
Publication status	Published - 1 Jan 2010
Externally published	Yes

Keywords

Arc discharge
Metal vapor
Pinch

ASJC Scopus subject areas

Physics and Astronomy(all)

Access to Document

10.3103/S1068335610010124

Fingerprint Dive into the research topics of 'The use of vacuum arc discharge as a load for XPG-1 high-current generator'. Together they form a unique fingerprint.

Cite this

@article{137dd6df5c1546909728d8f43508c2d0,

title = "The use of vacuum arc discharge as a load for XPG-1 high-current generator",

abstract = "It was attempted to use the vacuum arc discharge as a load of a high-current generator. The idea is as follows: metal vapor is injected using the vacuum arc discharge into a microgap of a load unit of the current generator. When the generator current flows over metal vapor, such a load begins to compress as in the classical Z pinch. During compression, Rayleigh-Taylor instabilities develop, which results in the formation of waists and hot spots. The hot spot radiation power can exceed the radiation power in the case of the X pinch used as a load by a factor of 1.5-2. The signal amplitude spread is significantly smaller than that when using the X pinch. The spectrum and sizes of the hot spot can be varied by selecting the mass and type of metal injected into the discharge region.",

keywords = "Arc discharge, Metal vapor, Pinch",

author = "Zhigalin, {A. S.} and Russkikh, {A. G.} and Oreshkin, {V. I.} and Shishlov, {A. V.} and Chaikovskii, {S. A.}",

year = "2010",

month = jan,

day = "1",

doi = "10.3103/S1068335610010124",

language = "English",

volume = "37",

pages = "29--30",

journal = "Bulletin of the Lebedev Physics Institute",

issn = "1068-3356",

publisher = "Springer Science + Business Media",

number = "1",

}

TY - JOUR

T1 - The use of vacuum arc discharge as a load for XPG-1 high-current generator

AU - Zhigalin, A. S.

AU - Russkikh, A. G.

AU - Oreshkin, V. I.

AU - Shishlov, A. V.

AU - Chaikovskii, S. A.

PY - 2010/1/1

Y1 - 2010/1/1

N2 - It was attempted to use the vacuum arc discharge as a load of a high-current generator. The idea is as follows: metal vapor is injected using the vacuum arc discharge into a microgap of a load unit of the current generator. When the generator current flows over metal vapor, such a load begins to compress as in the classical Z pinch. During compression, Rayleigh-Taylor instabilities develop, which results in the formation of waists and hot spots. The hot spot radiation power can exceed the radiation power in the case of the X pinch used as a load by a factor of 1.5-2. The signal amplitude spread is significantly smaller than that when using the X pinch. The spectrum and sizes of the hot spot can be varied by selecting the mass and type of metal injected into the discharge region.

AB - It was attempted to use the vacuum arc discharge as a load of a high-current generator. The idea is as follows: metal vapor is injected using the vacuum arc discharge into a microgap of a load unit of the current generator. When the generator current flows over metal vapor, such a load begins to compress as in the classical Z pinch. During compression, Rayleigh-Taylor instabilities develop, which results in the formation of waists and hot spots. The hot spot radiation power can exceed the radiation power in the case of the X pinch used as a load by a factor of 1.5-2. The signal amplitude spread is significantly smaller than that when using the X pinch. The spectrum and sizes of the hot spot can be varied by selecting the mass and type of metal injected into the discharge region.

KW - Arc discharge

KW - Metal vapor

KW - Pinch

UR - http://www.scopus.com/inward/record.url?scp=77953337470&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=77953337470&partnerID=8YFLogxK

U2 - 10.3103/S1068335610010124

DO - 10.3103/S1068335610010124

M3 - Article

AN - SCOPUS:77953337470

VL - 37

SP - 29

EP - 30

JO - Bulletin of the Lebedev Physics Institute

JF - Bulletin of the Lebedev Physics Institute

SN - 1068-3356

IS - 1

ER -