JPS60146418A - Vacuum bulb - Google Patents

Vacuum bulb

Info

Publication number
JPS60146418A
JPS60146418A JP31384A JP31384A JPS60146418A JP S60146418 A JPS60146418 A JP S60146418A JP 31384 A JP31384 A JP 31384A JP 31384 A JP31384 A JP 31384A JP S60146418 A JPS60146418 A JP S60146418A
Authority
JP
Japan
Prior art keywords
vacuum
contact
main electrode
electrode
low
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP31384A
Other languages
Japanese (ja)
Inventor
茂男 相馬
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP31384A priority Critical patent/JPS60146418A/en
Publication of JPS60146418A publication Critical patent/JPS60146418A/en
Pending legal-status Critical Current

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  • High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は真空しゃ断藷用真空バルブにかかシ特に低サー
ジ真空バルブの改良に関するものでらる。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to improvements in vacuum valves for vacuum isolation, particularly in low-surge vacuum valves.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

一般に真空パルプは10 Torr以下の真空中で電極
を開離し、真空のもつ曖れた消弧性と絶縁性を利用して
定流をしゃ断するものでらる。しかしその優れた消弧性
ゆえに、小−流しゃ断時、いわゆるさい新現象による過
大なザージ電圧の発生することも広く知られていること
でるる。この過大なサージ′祇圧の発生しない兵空バル
ブとして低サージ真空バルブがちる。その基本的な構成
を第1図に示す。
In general, vacuum pulp is produced by separating electrodes in a vacuum of 10 Torr or less and utilizing the ambiguous arc-extinguishing and insulating properties of vacuum to interrupt a constant flow. However, because of its excellent arc extinguishing properties, it is widely known that when a small current is interrupted, an excessive surge voltage is generated due to a so-called new phenomenon. A low-surge vacuum valve is used as a military/aircraft valve that does not generate this excessive surge pressure. Its basic configuration is shown in Figure 1.

第1図において真空パルプ1は両端開口をそれぞれ固定
端板3および可動端板4で10−’ Torr以下の真
空に密封した気密容器2の中に、固定側電極5および可
動側電極7がそれぞれ固定支持棒6および可動支持棒8
で支えられ図示しない操作機構によル、可動支持棒8を
介して開閉動作が行なわれる。9はベローズ、10はベ
ローズカバー、11はシールドでおる。
In FIG. 1, a vacuum pulp 1 has a fixed electrode 5 and a movable electrode 7 in an airtight container 2 whose openings at both ends are sealed to a vacuum of 10-' Torr or less by a fixed end plate 3 and a movable end plate 4, respectively. Fixed support rod 6 and movable support rod 8
Opening and closing operations are performed via a movable support rod 8 supported by an operating mechanism (not shown). 9 is a bellows, 10 is a bellows cover, and 11 is a shield.

固定側電極5および可動側電極7は、それぞれさい断電
流の低い接点材料、例えばAg −No材料よりなる接
点12および13と、電流しゃ断に寄与する。一般に脱
ガス処理を施された純鋼材料よシなる主電極部14.1
5で構成されている0また、主電極部14.15は、そ
のしゃ断する・−流に応じて、場合によっては磁気駆動
用の7゛岑が施されたものや縦磁界方式のコイル電極を
冶する主電極部で構成されたシする。
The fixed side electrode 5 and the movable side electrode 7 each contribute to current interruption with contacts 12 and 13 made of a contact material with a low cutting current, for example, an Ag-No material. Main electrode part 14.1 generally made of pure steel material subjected to degassing treatment
In addition, depending on the current to be cut off, the main electrode part 14.15 may be equipped with a 7mm diameter for magnetic drive or a vertical magnetic field type coil electrode. It consists of a main electrode section that conducts

このように構成された低サージ真空パルプのいちばんの
問題点は、そのしゃ断性能が25kA程度までしかない
ことである。これは、さい断電流の低い材料、そのもの
のしゃ断性能が一般のしゃ断器用に使用される接点材料
よりも悪いためであり、接点径を大きくしても思ったほ
どのしゃ断性能の向上がないためである。
The biggest problem with the low-surge vacuum pulp constructed in this way is that its breaking performance is only up to about 25 kA. This is because the material has a low breaking current and its breaking performance is worse than the contact material used for general circuit breakers, and even if the contact diameter is increased, the breaking performance does not improve as much as expected. It is.

〔発明の目的〕[Purpose of the invention]

本発明は、低サージでかつ大電流しや断が可能な真空パ
ルプを提供することを目的としている。
An object of the present invention is to provide a vacuum pulp that has low surges and can be cut by a large current.

〔発明の概要〕 本発明は、低サージ真空パルプにおいて、その電極部を
低さい新材料よシなる接点部および、純鋼材料ではない
、大電流しや所用材料よシなる電極部で構成される電極
を有するものであシ、従来の約1.6倍の40kA程度
の大電流しゃ断を可能としたものでちる。
[Summary of the Invention] The present invention provides a low-surge vacuum pulp in which the electrode part is made of a low-density new material, and the electrode part is made of a high-current material other than pure steel. It is possible to cut off a large current of about 40 kA, which is about 1.6 times that of the conventional one.

〔発明の実施例〕[Embodiments of the invention]

本発明の一実施例を第2図に示す。 An embodiment of the present invention is shown in FIG.

第2図は縦磁界方式に応用した場合を示すが、第2図の
コイルば極を1余き、゛ト4極部にうず巻状の溝を施す
と、磁気駆動方式となることは周知の通夛である。
Figure 2 shows the case where it is applied to the vertical magnetic field system, but it is well known that if a spiral groove is formed on the coil poles in Figure 2 and the four poles, a magnetic drive system will be obtained. This is a common practice.

また第2図には、電極部分のみを示すが他の部分は略渠
1図と同一であるので省略する。
Further, in FIG. 2, only the electrode portion is shown, but the other portions are substantially the same as in FIG. 1 and are therefore omitted.

第21において、固定・−極20および可動電極21は
、それぞれ次のようIF:、構成される。22 、23
はそれぞれ低さい新材料、例えばAg−〜vC材料より
なる接点であシ、後述する主電極、補助゛一極と比較し
、凸状に形成される。また24.25は主電極でらシ、
純銅を除く大電流しやljt用材料、例えば0u−Te
系合金、Ou −Bi系合金、Ou −Pb系合金、O
u −Or系合金等の材料よシなる。26 、27は補
助電極で必シ、一般に純鋼材料よりなる。これは接点、
主電極、コイル電極のロウ付性が悪い場合に使用する必
要がらシ、特に必要がない材料の場合は、主電極が補助
電極を兼用することもある。
In the twenty-first, the fixed/-pole 20 and the movable electrode 21 are each configured as follows. 22, 23
are contacts made of a new material with low thickness, for example, Ag--vC material, and are formed in a convex shape compared to the main electrode and the auxiliary single pole, which will be described later. Also, 24.25 is the main electrode,
Materials for large current shields other than pure copper, such as 0u-Te
alloy, Ou-Bi alloy, Ou-Pb alloy, O
It depends on materials such as u-Or alloys. Reference numerals 26 and 27 are auxiliary electrodes, which are generally made of pure steel. This is a contact point,
It is necessary to use it when the main electrode and coil electrode have poor brazing properties, but when the material is not particularly necessary, the main electrode may also serve as an auxiliary electrode.

28.29は縦磁界発生用のコイル電極であシ、シゃ断
電流に必要な磁界強度を副整するために、適宜分割数が
決められる。30.31は固定′−一極持棒、および可
動電極支持棒で必シ、真空パルプ外部への電流通路とな
る。
28 and 29 are coil electrodes for generating a longitudinal magnetic field, and the number of divisions is appropriately determined in order to sub-adjust the magnetic field strength required for the cutoff current. Reference numerals 30 and 31 are a fixed single-pole support rod and a movable electrode support rod, which necessarily serve as a current path to the outside of the vacuum pulp.

このように構成された真空パルプによると、まず小電流
しゃ断の場合、低さい断′亀流を有する材料にて発弧さ
せること、および100Å以下の小電流の場合、真空ア
ークスポットが略1個しか生成されず、スポット自身の
動きがないこと等によ勺′この低さい新材料に維持され
るため、さい断による過電圧の発生が防止できることと
なる。
According to the vacuum pulp constructed in this way, firstly, in the case of a small current interruption, the arc should be caused by a material with a low breaking current, and in the case of a small current of 100 Å or less, there will be approximately one vacuum arc spot. Since only a small amount of the new material is generated and the spot itself does not move, the new material is maintained at a relatively low temperature, thereby making it possible to prevent overvoltage from occurring due to cutting.

次に大電流しゃ断の場合は、やはり低さい新材料を有す
る接点部分で発弧させるが、電流が大きいため多数のス
ポットが生成され自動的に拡散される。このとき主電極
24.25が前記したような純鋼材で形成されている場
合は接点部分との蒸気圧の差(より、アークはほとんど
拡散されず、大部分が接点部分VC集中したような形態
を示す。しかし、純鋼材料よシも蒸気圧の高い例えば0
u−Bi系合金、Ou −Te系合金、Ou −Pb系
合金、0u−Or系合金等の材料を使用することによシ
、その蒸気圧の差が小さくなることから、アークがほぼ
電極全面に拡散し、電極径に比例したしゃ断性能が得ら
れることとなる。
Next, in the case of large current interruption, the arc is fired at the contact part with the new material, which is also low, but because the current is large, many spots are generated and automatically diffused. At this time, if the main electrodes 24 and 25 are made of pure steel as described above, there is a difference in vapor pressure between them and the contact portions (because of this, the arc is hardly diffused and most of the VC is concentrated in the contact portions). However, pure steel materials also have high vapor pressure, such as 0
By using materials such as u-Bi alloy, Ou-Te alloy, Ou-Pb alloy, Ou-Or alloy, etc., the difference in vapor pressure becomes smaller, so the arc spreads over almost the entire electrode surface. This results in a blocking performance proportional to the electrode diameter.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、接点部を低さい断電流を鳴する材料で
形成し、主電極部を純銅材料でない、例えばOu −T
e系、Ou −Bi系、Ou 7 Pb系、Ou −O
r系合金よシなる大電流しや所用材料にて形成した電極
部とすることにより25kA以上の大電流しゃ断性能を
有する低サージ真空パルプを得ることができる。
According to the present invention, the contact portion is formed of a material that produces a low breaking current, and the main electrode portion is formed of a material other than pure copper, such as Ou-T.
e series, Ou-Bi series, Ou7Pb series, Ou-O
A low-surge vacuum pulp having a large current breaking performance of 25 kA or more can be obtained by forming the electrode part from a material suitable for large currents such as r-based alloys.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来の低サージ真空パルプを示す断面図、第2
図は本発明の一実施例を示す一極部分の断面図である。 22.23・・・接点 24 、25・・・王1!極 (7317)代理人弁理士 則 近 憲 佑 (ほか1
名)第1図 !
Figure 1 is a cross-sectional view showing conventional low-surge vacuum pulp, Figure 2
The figure is a sectional view of a single pole portion showing an embodiment of the present invention. 22.23...Contact points 24, 25...King 1! Goku (7317) Representative Patent Attorney Noriyuki Chika (and 1 others)
Name) Figure 1!

Claims (2)

【特許請求の範囲】[Claims] (1)真空容器内に接点とこの接点を中央にロー付によ
シ取9付けた主電極からなる少なくとも1対の互いに接
離し得る電極を設けた真空パルプにおいて、前記接点を
低さい断電流を有する材料で形成し、その周辺の主電極
部分を、0u−Te系、Ou −Bi系、Ou −Pb
系、On −Or系合金より選択される一種類の材料に
より形成したことを特徴とする真空しゃ断器用真空バル
ブ。
(1) In vacuum pulp, in which at least one pair of electrodes that can be brought into contact with and separated from each other, consisting of a contact and a main electrode with a soldered bolt 9 attached to the center of the contact, is provided in a vacuum container, the contact is connected to a low breaking current. The main electrode part around the main electrode is made of a material having Ou-Te system, Ou-Bi system, Ou-Pb system.
1. A vacuum valve for a vacuum breaker, characterized in that it is made of one type of material selected from On-Or type and On-Or type alloys.
(2)主電極部分に、アークに対して軸方向の磁界を印
加するためのコイル電極を備えたことを特徴とする特許
請求の範囲第1項記載の真空パルプ。
(2) The vacuum pulp according to claim 1, wherein the main electrode portion includes a coil electrode for applying an axial magnetic field to the arc.
JP31384A 1984-01-06 1984-01-06 Vacuum bulb Pending JPS60146418A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31384A JPS60146418A (en) 1984-01-06 1984-01-06 Vacuum bulb

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31384A JPS60146418A (en) 1984-01-06 1984-01-06 Vacuum bulb

Publications (1)

Publication Number Publication Date
JPS60146418A true JPS60146418A (en) 1985-08-02

Family

ID=11470420

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31384A Pending JPS60146418A (en) 1984-01-06 1984-01-06 Vacuum bulb

Country Status (1)

Country Link
JP (1) JPS60146418A (en)

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