JPH08222089A - Vacuum bulb - Google Patents

Vacuum bulb

Info

Publication number
JPH08222089A
JPH08222089A JP2241195A JP2241195A JPH08222089A JP H08222089 A JPH08222089 A JP H08222089A JP 2241195 A JP2241195 A JP 2241195A JP 2241195 A JP2241195 A JP 2241195A JP H08222089 A JPH08222089 A JP H08222089A
Authority
JP
Japan
Prior art keywords
electrode
current
highly conductive
magnetic field
conductivity
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
JP2241195A
Other languages
Japanese (ja)
Inventor
Seiichi Nakamura
誠一 中村
Mitsutaka Honma
三孝 本間
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 JP2241195A priority Critical patent/JPH08222089A/en
Publication of JPH08222089A publication Critical patent/JPH08222089A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE: To enhance the carrying-current without enlarging the outer form by forming at least one of a fixed electrode and a movable electrode by impregnating a highly conductive part consisting of a highly conductive material with a material lower in conductivity than it. CONSTITUTION: At least one of a fixed electrode and a movable electrode is formed by impregnating a highly conductive coil electrode with a material slightly lower in conductivity than it. Namely, an impregnated part 1b impregnated with the material slightly lower in conductivity than a highly conductive part 1a is formed between a current-carrying shaft 4 and a contact 2. The part 1a is, for example, formed of copper, and an alloy lower in conductivity than copper such as silver-copper alloy is impregnated in the space part, whereby an electrode 1 is formed. At current-carrying, a large current can be carried since the current is carried to the whole electrode, while the large current can be interrupted with a small electrode at interruption since the interrupting performance is enhanced by forming a longitudinal magnetic field or vertical magnetic field.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、電極の構造と材料を改
良した真空バルブに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a vacuum valve having an improved electrode structure and material.

【0002】[0002]

【従来の技術】従来の真空遮断器に用いられる真空バル
ブの構成を図7に示す。図7において、真空バルブ10
は、絶縁円筒11の両端を固定フランジ12と可動フランジ
13で封止して形成された真空容器の内部に、固定電極14
と可動電極15が接離可能に配設されて構成している。
2. Description of the Related Art The structure of a vacuum valve used in a conventional vacuum circuit breaker is shown in FIG. In FIG. 7, the vacuum valve 10
Both ends of the insulating cylinder 11 are fixed flange 12 and movable flange
A fixed electrode 14 is placed inside the vacuum container sealed with 13.
And the movable electrode 15 are arranged so that they can come into contact with and separate from each other.

【0003】このうち、固定電極14は、固定フランジ12
を気密に貫通した固定軸16の先端に一面をろう付で固定
され他面に接触子21を有しており、真空容器の外部とは
この固定軸16の上端を介して接続される。一方、可動電
極15は、断面逆U字状のベローズカバー19を気密に貫通
した可動軸17の先端にろう付で固定されており、真空容
器の外部とはこの可動軸17の下端を介して接続される。
Of these, the fixed electrode 14 is the fixed flange 12
One end is fixed to the tip of a fixed shaft 16 that penetrates in an airtight manner by brazing, and a contact 21 is provided on the other surface, and the outside of the vacuum container is connected through the upper end of the fixed shaft 16. On the other hand, the movable electrode 15 is fixed by brazing to the tip of a movable shaft 17 that penetrates airtightly through a bellows cover 19 having an inverted U-shaped cross section, and is connected to the outside of the vacuum container via the lower end of the movable shaft 17. Connected.

【0004】また、この可動軸17は、可動フランジ13と
ベローズカバー19間にろう付されたベローズ18と、可動
フランジ13の中心に挿入された断面凸字状のガイド20を
介して可動フランジ13に支えられており、真空容器内の
真空を維持した状態で可動軸17の下端に連結される図示
しない操作機構部によって、矢印Bで示すように駆動さ
れることで、電極の接離を可能にしている。
The movable shaft 17 has a bellows 18 brazed between the movable flange 13 and a bellows cover 19, and a guide 20 having a convex cross-section inserted at the center of the movable flange 13 to move the movable flange 13. It is supported by and is driven by an operation mechanism portion (not shown) connected to the lower end of the movable shaft 17 while maintaining the vacuum in the vacuum container, so that the electrodes can be brought into and out of contact with each other. I have to.

【0005】ところで、真空バルブは、周知のように、
真空の優れた絶縁耐力を利用しているため、例えば、六
フッ化硫黄ガスなどの絶縁媒体を使ったガス遮断器に比
べて、電極間の間隙を狭くでき、外径を小形にすること
ができる。また、遮断容量も、電極の構造を改良するこ
とで増やすことができる。
By the way, as is well known, the vacuum valve is
Since the excellent dielectric strength of vacuum is used, the gap between the electrodes can be made smaller and the outer diameter can be made smaller than that of a gas circuit breaker that uses an insulating medium such as sulfur hexafluoride gas. it can. Also, the breaking capacity can be increased by improving the structure of the electrode.

【0006】真空バルブの遮断性能を上げるための一手
段としては、電極間に発生するアークによる電極の局部
加熱を抑える方法がある。つまり、局部加熱による異常
な荷電粒子の発生を抑えることにより、アークの発生を
抑えて遮断性能を向上させる。このための電極構造とし
ては、電極間に発生するアークに平行に磁界を印加する
方法と、アークに対して直交方向に磁界を印加する方法
がある。
As one means for improving the breaking performance of the vacuum valve, there is a method of suppressing local heating of the electrodes due to an arc generated between the electrodes. That is, by suppressing the generation of abnormal charged particles due to local heating, the generation of arcs is suppressed and the breaking performance is improved. As an electrode structure for this purpose, there are a method of applying a magnetic field parallel to the arc generated between the electrodes and a method of applying a magnetic field in a direction orthogonal to the arc.

【0007】このうち、アークに平行に磁界を印加する
方法を採用した電極には、いわゆる縦磁界電極構造があ
る。この方法は、電極間に発生するアークを、磁界の効
果により電極全体に分散させて、遮断性能を上げる方法
である。一方、アークに対して直交する磁界を印加する
方法を採用した電極には、いわゆるスパイラル電極があ
る。この方法は、大電流遮断時に電極面に集中したアー
クを、電極表面で回転させて遮断性能を上げる方法であ
る。つまり、集中したアークを移動させることにより、
電極の局部加熱による接点の部分的溶融を防いで、遮断
性能を上げる方法である。これらはいずれの電極も磁界
によりアークを制御するため、電極に電流を回転させて
流すための溝が設けられていた。
Among them, an electrode adopting a method of applying a magnetic field parallel to an arc has a so-called longitudinal magnetic field electrode structure. In this method, the arc generated between the electrodes is dispersed over the entire electrode by the effect of the magnetic field to improve the breaking performance. On the other hand, there is a so-called spiral electrode as an electrode adopting a method of applying a magnetic field orthogonal to an arc. This method is a method in which an arc concentrated on the electrode surface when a large current is cut off is rotated on the electrode surface to improve the breaking performance. In other words, by moving the concentrated arc,
This is a method of improving the breaking performance by preventing partial melting of the contacts due to local heating of the electrodes. Since all of these electrodes control the arc by a magnetic field, the electrodes were provided with a groove for rotating and flowing an electric current.

【0008】[0008]

【発明が解決しようとする課題】ところが、このような
従来の真空バルブは、アーク制御のため電極が複雑にな
り、通電面積が断面積の割りに小さくなる一方で、通電
電流を大きくするためには、通電時の発熱をおさえるた
め断面積をさらに大きくする必要があった。そこで本発
明の目的は、外形(断面積)を大きくすることなく、通
電電流を大きくすることのできる真空バルブを得ること
を目的とする。
However, in such a conventional vacuum valve, the electrodes are complicated due to arc control, and the current-carrying area is reduced relative to the cross-sectional area, while the current-carrying current is increased. Had to further increase the cross-sectional area in order to suppress heat generation during energization. Therefore, an object of the present invention is to provide a vacuum valve capable of increasing the energizing current without increasing the outer shape (cross-sectional area).

【0009】[0009]

【課題を解決するための手段】本発明は、通電軸を介し
て外部と接続される固定電極と可動電極が真空容器内に
接離可能に収納された真空パルブの、固定電極と可動電
極のうちの少なくとも一方を、導電性の高いコイル電極
をこれよりやや低い材料で含浸して形成することを特徴
とするものである。電極は縦磁界電極、円盤に溝を入れ
たスパイラルやコントレート,コイル線などにより形成
され、これらを銅コバルトなどにより含浸して形成され
る。
SUMMARY OF THE INVENTION The present invention relates to a fixed electrode and a movable electrode of a vacuum valve in which a fixed electrode and a movable electrode, which are connected to the outside via a current-carrying shaft, are housed in a vacuum container so that they can come into contact with and separate from each other. It is characterized in that at least one of them is formed by impregnating a coil electrode having high conductivity with a material slightly lower than this. The electrodes are formed by a vertical magnetic field electrode, a spiral having a groove in a disk, a contact, a coil wire, or the like, and impregnated with copper cobalt or the like.

【0010】[0010]

【作用】本発明においては、電極が接触し、電流が流れ
ている時(通電時)は、導電率の差はあるが電極全体に
電流が流れ、電極の温度上昇は抑制される。また電流を
切る(電極が離れる)電流遮断時には、電流が絞られ導
電率の高い高導電部にほとんどの遮断電流が流れること
により、コイル電極を用いた場合には、電極間に発生す
るアークに平行に磁界を印加し、スパイラル電極を用い
た場合には電極間に流れるアークに直交方向に磁界を印
加する。さらにコイル線を用いた場合には巻数を変える
ことにより容易に遮断時の電極間磁界の強さを可変する
ことができる。
In the present invention, when the electrodes are in contact with each other and a current is flowing (current is flowing), a current flows through the entire electrode although there is a difference in conductivity, and the temperature rise of the electrode is suppressed. In addition, when the current is cut off (the electrodes are separated), most of the cutoff current flows in the high-conductivity area where the current is narrowed and the conductivity is high. A magnetic field is applied in parallel, and when a spiral electrode is used, a magnetic field is applied in an orthogonal direction to the arc flowing between the electrodes. Furthermore, when a coil wire is used, the strength of the inter-electrode magnetic field at the time of interruption can be easily changed by changing the number of turns.

【0011】[0011]

【実施例】以下、本発明の真空バルブの第一実施例を図
面を参照して説明する。なお真空バルブ全体の構造は、
図7と同一のため、電極の構造について、図1ないし図
6を用いて詳細に説明する。また電極は可動側,固定側
とも全く同一構造なので、一方についてのみ説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A first embodiment of the vacuum valve of the present invention will be described below with reference to the drawings. The structure of the entire vacuum valve is
Since it is the same as FIG. 7, the structure of the electrode will be described in detail with reference to FIGS. 1 to 6. Further, since the electrodes have the same structure on both the movable side and the fixed side, only one of them will be described.

【0012】図1,図2は、電流遮断時に、電極間に発
生するアークに平行に磁界を印加する縦磁界電極を高導
電部に使用した例である。ここで図2は含浸前の高導電
部1aとこれに取付けられる接触子2、補強軸3、通電
軸4を示したものである。図1は、この通電軸4から接
触子2までの間を高導電部1aの導電率よりやや低い材
料により含浸した含浸部1bを有する。
FIGS. 1 and 2 show an example in which a longitudinal magnetic field electrode for applying a magnetic field parallel to an arc generated between the electrodes when the current is cut off is used in the highly conductive portion. Here, FIG. 2 shows the high-conductivity portion 1a before impregnation, the contactor 2, the reinforcing shaft 3, and the current-carrying shaft 4 attached thereto. FIG. 1 has an impregnated portion 1b in which the portion between the current-carrying shaft 4 and the contactor 2 is impregnated with a material having a slightly lower conductivity than the high conductive portion 1a.

【0013】例えば高導電部は銅により形成し、空間部
分に銀銅合金等の銅より導電率の低い合金を含浸させる
ことにより電極を形成する。また、コイル電極又はスパ
イラル電極を形成した後にクロム等の金属粉体を充填し
た後焼結処理を行い電極を形成する。あるいは銅コバル
ト(CuCo)を含浸しても良い。
For example, the highly conductive portion is formed of copper, and the electrode is formed by impregnating the space portion with an alloy having a lower conductivity than copper, such as a silver-copper alloy. Further, after forming a coil electrode or a spiral electrode, metal powder such as chromium is filled and then sintering is performed to form an electrode. Alternatively, copper cobalt (CuCo) may be impregnated.

【0014】この様に構成された真空バルブにおいて
は、電極が接触し電流が流れている通電時は、導電率の
部分的(相違)差はあるが、電極全体に電流が流れ、電
極の温度上昇は抑制される。
In the vacuum valve having such a structure, when the electrodes are in contact with each other and a current flows, there is a partial (difference) difference in conductivity, but a current flows through the entire electrode and the temperature of the electrode changes. The rise is suppressed.

【0015】また電流を切る遮断時には、電流が絞ら
れ、導電率の高い(良い)コイル電極にほとんどの遮断
電流が流れ、電極間に発生するアークに平行に磁界を印
加し、アークを電極面に均等にする。
When the current is cut off, the current is narrowed, and most of the cutoff current flows through the coil electrodes having high conductivity (good), and a magnetic field is applied in parallel to the arc generated between the electrodes, so that the arc is directed to the electrode surface. Evenly.

【0016】図3,図4は、第2実施例であり、図1お
よび図2の縦磁界電極のかわりに螺旋状のコイル線1c
を高導電部に用いたものである。この様に構成された電
極による真空バルブも第1実施例と同様の作用効果があ
り、さらに、コイル線の巻数を変えることにより容易に
遮断時の電極間磁界の強さを可変することができ、アー
クの均等化をも可変できる。
FIGS. 3 and 4 show a second embodiment, in which a spiral coil wire 1c is used instead of the longitudinal magnetic field electrodes shown in FIGS.
Is used for the high conductivity part. The vacuum valve with electrodes constructed in this way has the same effects as the first embodiment, and the strength of the inter-electrode magnetic field at the time of interruption can be easily changed by changing the number of turns of the coil wire. The arc equalization can also be changed.

【0017】図5は、電流遮断時に電極間に発生するア
ークに直交する磁界を印加するスパイラル電極を高導電
部に用いた実施例で、接触子2、スパイラル電極1c、
通電軸4とこの通電軸4から接触子2までの間を、スパ
イラル電極1d導電率よりやや低い材料で含浸した含浸
部1bからなる。さらに図6はコントレート電極を高導
電部に用いた場合の例であり、電極1はコントレート電
極1eとこの含浸部1bとから成る。
FIG. 5 shows an embodiment in which a spiral electrode for applying a magnetic field orthogonal to the arc generated between the electrodes when the current is cut off is used in the highly conductive portion. The contact 2, the spiral electrode 1c,
The current-carrying shaft 4 and a portion between the current-carrying shaft 4 and the contact 2 are made of an impregnated portion 1b in which the spiral electrode 1d is impregnated with a material having a slightly lower conductivity. Further, FIG. 6 shows an example in which a contact electrode is used for the high conductivity portion, and the electrode 1 is composed of the contact electrode 1e and the impregnated portion 1b.

【0018】これらのスパイラル電極,コントレート電
極を用いた場合には、電極が接触し電流が流れている通
電時は、導電率の部分的差があるものの、電極全体に電
流が流れ電極の温度上昇は抑制される。また電流を切る
遮断時には、電流が絞られ導電率の高い部分にほとんど
の遮断電流が流れ、電極間に発生するアークに直交方向
に磁界を発生し、アークを電極面で移動させる。
When these spiral electrodes and control electrodes are used, when the electrodes are in contact with each other and a current is flowing, there is a partial difference in conductivity, but a current flows through the entire electrode, and the temperature of the electrode changes. The rise is suppressed. Further, when the current is cut off, most of the cutoff current flows in a portion where the current is narrowed and the conductivity is high, a magnetic field is generated in a direction orthogonal to the arc generated between the electrodes, and the arc is moved on the electrode surface.

【0019】[0019]

【発明の効果】本発明によれば、通電時は電極全体に電
流が流れるため大電流通電が可能になり、遮断時には、
縦磁界または垂直磁界をつくることにより遮断性能が良
くなるため、小さい電極で大電流遮断が可能となる。
According to the present invention, since a current flows through the entire electrode during energization, a large current can be energized, and during interruption,
Since the breaking performance is improved by creating a vertical magnetic field or a vertical magnetic field, it is possible to cut a large current with a small electrode.

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

【図1】縦磁界電極を用いた場合の本発明の一実施例の
(a)平面図,(b)正面図。
FIG. 1A is a plan view and FIG. 1B is a front view of an embodiment of the present invention when a vertical magnetic field electrode is used.

【図2】縦磁界電極を用いた場合の本発明の一実施例の
組立図。
FIG. 2 is an assembly view of an embodiment of the present invention in which a vertical magnetic field electrode is used.

【図3】コイル線を用いた本発明の一実施例の(a)平
面図,(b)正面図。
3A is a plan view and FIG. 3B is a front view of an embodiment of the present invention using a coil wire.

【図4】コイル線を用いた本発明の一実施例の斜視図。FIG. 4 is a perspective view of an embodiment of the present invention using a coil wire.

【図5】スパイラル電極を用いた本発明の一実施例の
(a)平面図,(b)正面図。
5 (a) is a plan view and FIG. 5 (b) is a front view of an embodiment of the present invention using a spiral electrode.

【図6】コントレート電極を用いた本発明の一実施例の
斜視図。
FIG. 6 is a perspective view of an embodiment of the present invention using a contact electrode.

【図7】一般的な真空バルブの構成を示す縦断面図。FIG. 7 is a vertical cross-sectional view showing the configuration of a general vacuum valve.

【符号の説明】[Explanation of symbols]

1…電極、 1a…縦磁界電極(高導電部)、
1b…含浸部、1c…コイル線電極、 1d…ス
パイラル電極、1e…コントレート電極、 2…接
触子、 3…補強軸、4…通電軸
1 ... Electrode, 1a ... Longitudinal magnetic field electrode (highly conductive portion),
1b ... Impregnation part, 1c ... Coil wire electrode, 1d ... Spiral electrode, 1e ... Contact electrode, 2 ... Contactor, 3 ... Reinforcing shaft, 4 ... Energizing shaft

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 通電軸を介して外部と接続される固定電
極と可動電極が真空容器内に接離可能に収納された真空
バルブにおいて、これらの固定電極と可動電極の少なく
とも一方の電極を、導電性の高い材料で形成された高導
電部をこれより導電性の低い材料で含浸して形成したこ
とを特徴とする真空バルブ。
1. A vacuum valve in which a fixed electrode and a movable electrode, which are connected to the outside through an energizing shaft, are housed in a vacuum container so that they can be contacted and separated, at least one of the fixed electrode and the movable electrode is A vacuum valve, which is formed by impregnating a highly conductive portion made of a highly conductive material with a material having a lower electrical conductivity.
【請求項2】 前記高導電部を縦磁界電極により形成し
たことを特徴とする請求項1に記載の真空バルブ。
2. The vacuum valve according to claim 1, wherein the highly conductive portion is formed by a vertical magnetic field electrode.
【請求項3】 前記高導電部を円盤に溝を入れて形成し
たことを特徴とする請求項1に記載の真空バルブ。
3. The vacuum valve according to claim 1, wherein the highly conductive portion is formed by forming a groove in a disk.
【請求項4】 前記高導電部をコイル線により形成した
ことを特徴とする請求項1に記載の真空バルブ。
4. The vacuum valve according to claim 1, wherein the highly conductive portion is formed by a coil wire.
【請求項5】 前記高導電部を銅コバルト(CuCo)
により含浸することを特徴とする請求項1ないし請求項
4に記載の真空バルブ。
5. The high conductivity portion is copper cobalt (CuCo).
The vacuum valve according to any one of claims 1 to 4, wherein the vacuum valve is impregnated with.
JP2241195A 1995-02-10 1995-02-10 Vacuum bulb Pending JPH08222089A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2241195A JPH08222089A (en) 1995-02-10 1995-02-10 Vacuum bulb

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2241195A JPH08222089A (en) 1995-02-10 1995-02-10 Vacuum bulb

Publications (1)

Publication Number Publication Date
JPH08222089A true JPH08222089A (en) 1996-08-30

Family

ID=12081933

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2241195A Pending JPH08222089A (en) 1995-02-10 1995-02-10 Vacuum bulb

Country Status (1)

Country Link
JP (1) JPH08222089A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020054128A1 (en) * 2018-09-14 2020-03-19 株式会社日立製作所 Gas-insulated switching device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020054128A1 (en) * 2018-09-14 2020-03-19 株式会社日立製作所 Gas-insulated switching device
JP2020048252A (en) * 2018-09-14 2020-03-26 株式会社日立製作所 Gas-insulation opening/closing device

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