JPH0822751A - Vacuum valve - Google Patents

Vacuum valve

Info

Publication number
JPH0822751A
JPH0822751A JP15775494A JP15775494A JPH0822751A JP H0822751 A JPH0822751 A JP H0822751A JP 15775494 A JP15775494 A JP 15775494A JP 15775494 A JP15775494 A JP 15775494A JP H0822751 A JPH0822751 A JP H0822751A
Authority
JP
Japan
Prior art keywords
electrode
current
contactor
grooves
vacuum valve
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
JP15775494A
Other languages
Japanese (ja)
Inventor
Hiromichi Somei
宏通 染井
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 JP15775494A priority Critical patent/JPH0822751A/en
Publication of JPH0822751A publication Critical patent/JPH0822751A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To stabilize breaking capacity regardless of an arc generating point at electric current breaking time by providing current-carrying parts in parts where an angle formed by grooves arranged on a side surface of an electrode and a contactor side end surface of a cylindrical electrode is an acute angle. CONSTITUTION:A movable electrode 3B is installed on the tip of a movable current-carrying shaft 5B, and a layer composed of current-carrying parts 21a to 21d and insulating parts 8a to 8d is arranged in a front part of the electrode 3B. A contactor 4B is fixed to the front surface, and grooves 6a to 6d are formed in a cylinder part of this electrode 3B, and are formed so as to continue with grooves 7a to 7d formed in a bottom part. Between the cylinder part of the electrode 3B and the contactor 4B, Current-carrying parts 21a to 21d are arranged in parts on the side where an angle formed by the grooves 7a to 7d and a cylinder part end surface is an acute angle, and a part except it becomes the insulating parts 8a to 8d. Then, an electric current flows to the contactor 4B from the movable current-carrying shaft 5B through the cylinder part. This electric current has a circumferential directional component, and generates a sufficient axial directional magnetic field, and stable and excellent breaking performance is obtained.

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、真空バルブに関する。FIELD OF THE INVENTION This invention relates to vacuum valves.

【0002】[0002]

【従来の技術】真空遮断器に組み込まれる従来の縦磁界
電極を備えた真空バルブの縦断面図を図3に、この図3
のB−B断面図を図4に示す。従来の真空バルブは、図
3及び図4に示すように、絶縁円筒1の両端を固定フラ
ンジ2A及び可動フランジ2Bで密閉された真空容器内
に、固定電極13Aと可動電極13Bが接離可能に配置され
ている。
2. Description of the Related Art FIG. 3 is a vertical sectional view of a conventional vacuum valve having a vertical magnetic field electrode incorporated in a vacuum circuit breaker.
4 is a sectional view taken along line BB of FIG. As shown in FIGS. 3 and 4, the conventional vacuum valve allows the fixed electrode 13A and the movable electrode 13B to come into contact with and separate from each other in a vacuum container in which both ends of the insulating cylinder 1 are sealed by the fixed flange 2A and the movable flange 2B. It is arranged.

【0003】このうち、固定電極13Aは、固定フランジ
2Aを貫通した固定通電軸5Aの先端に固着され、この
固定電極13Aの前面には接触子4Aが結合され、真空容
器の外部とは固定通電軸5Aで接続されている。一方、
可動電極13Bは、可動フランジ2Bに貫設された案内管
10を貫通した可動通電軸5Bの先端に固着され、この可
動電極13Bの前面には接触子4Bが結合され、真空容器
の外部とは可動通電軸5Bで接続されている。また、こ
の可動通電軸5Bの中間部は、ベローズカバー15とベロ
ーズ9を介して可動フランジ2Bに支持されており、真
空容器内の真空を維持した状態で可動通電軸5Bの下端
に連結された絶縁ロッドを介して図示しない操作機構部
によって、固定電極13Aとの接離による通電と遮断を可
能にしている。絶縁円筒1の内面には、円筒状のアーク
シールド14が取り付けられている。
Of these, the fixed electrode 13A is fixed to the tip of a fixed current-carrying shaft 5A which penetrates the fixed flange 2A, and a contactor 4A is coupled to the front surface of the fixed electrode 13A so as to be fixed to the outside of the vacuum vessel. It is connected by a shaft 5A. on the other hand,
The movable electrode 13B is a guide tube penetrating the movable flange 2B.
It is fixed to the tip of the movable energizing shaft 5B penetrating 10 and the contactor 4B is coupled to the front surface of the movable electrode 13B, and is connected to the outside of the vacuum container by the movable energizing shaft 5B. The intermediate portion of the movable energizing shaft 5B is supported by the movable flange 2B via the bellows cover 15 and the bellows 9 and is connected to the lower end of the movable energizing shaft 5B while maintaining the vacuum in the vacuum container. An operation mechanism portion (not shown) via the insulating rod enables energization and interruption by contact and separation with the fixed electrode 13A. A cylindrical arc shield 14 is attached to the inner surface of the insulating cylinder 1.

【0004】ところで、真空バルブは、真空の優れた絶
縁耐力を利用しているため、他の絶縁媒体を使用した例
えばSF6 ガス遮断器に比べて、電極間距離を短くする
ことができ、外形を小形にすることができる。また、遮
断容量においても、電極の構成を変えることで増やすこ
とができる。一方、真空バルブの遮断性能を上げるため
には、電極間に発生するアークによる電極の局部加熱を
抑える必要がある。つまり、電極の局部加熱による異常
な荷電粒子の発生と金属蒸気の発生を抑えることで、遮
断性能を上げることができる。このための電極構造とし
ては、電流遮断時に電極間に発生するアークに対して、
磁界で電磁力を加える方法が一般的である。
By the way, since the vacuum valve utilizes the excellent dielectric strength of vacuum, the distance between the electrodes can be shortened as compared with, for example, an SF 6 gas circuit breaker using another insulating medium, and the outer shape can be reduced. Can be made small. Also, the breaking capacity can be increased by changing the configuration of the electrodes. On the other hand, in order to improve the breaking performance of the vacuum valve, it is necessary to suppress the local heating of the electrodes due to the arc generated between the electrodes. That is, the blocking performance can be improved by suppressing the generation of abnormal charged particles and the generation of metal vapor due to local heating of the electrode. The electrode structure for this is as follows:
A method of applying an electromagnetic force with a magnetic field is common.

【0005】磁界の印加方向の一つとして、電極間に発
生するアークに対して、直行する磁界を印加する方法が
ある。この方法を採用した電極は、一般にスパイラル電
極およびコントレート電極と呼ばれているが、このよう
な電極で発生する磁界は、電極の軸心から放射状の磁界
である。したがって、電極間に発生したアークに対し
て、直行する磁界となるため、アークには円周方向にロ
ーレンツ力が働く。この結果、アークは円周方向に回転
駆動され、電極表面を移動させることで、局部的な熱入
力による電極の局部的な溶融による前述の粒子と蒸気の
発生を防ぐことができる。
As one of the application directions of the magnetic field, there is a method of applying a perpendicular magnetic field to the arc generated between the electrodes. The electrodes adopting this method are generally called spiral electrodes and contract electrodes, but the magnetic field generated by such electrodes is a magnetic field radial from the axial center of the electrodes. Therefore, since the magnetic field is orthogonal to the arc generated between the electrodes, Lorentz force acts on the arc in the circumferential direction. As a result, the arc is rotationally driven in the circumferential direction, and by moving the electrode surface, it is possible to prevent the aforementioned generation of particles and vapor due to local melting of the electrode due to local heat input.

【0006】ことろが、高電圧の回路に適用される真空
遮断器に組み込まれる真空バルブでは、電極間の耐電圧
値を上げるために、電極間距離を増やす必要があるが、
この電極間に発生するアークに対して直行する磁界を印
加する上述の電極構造では、アークが電極表面を回転す
るときに、アークが円周方向に伸ばされ、電極から放射
状に飛び出すおそれがある。この場合、アークが電極の
周囲に取り付けられているアークシールドへ点弧するお
それもあり、その際にはアークはその点弧部に停滞し、
局部的に過大な熱入力が発生する。この過大な熱入力で
電極とアークシールドが溶融すると、遮断性能が低下す
る。さらに、この電極構造では、前述したように、アー
クの状態は集中アークで高温のため、接触子の消耗が加
速され、大電流遮断時の開閉寿命が低下する。
In a vacuum valve incorporated in a vacuum circuit breaker applied to a high voltage circuit, it is necessary to increase the distance between the electrodes in order to increase the withstand voltage value between the electrodes.
In the above electrode structure in which a magnetic field perpendicular to the arc generated between the electrodes is applied, when the arc rotates on the surface of the electrode, the arc may be stretched in the circumferential direction and may be radially ejected from the electrode. In this case, there is a risk that the arc will ignite the arc shield mounted around the electrode, in which case the arc will stagnate at the ignition part,
Excessive heat input is generated locally. If the electrode and the arc shield are melted by this excessive heat input, the breaking performance is deteriorated. Further, in this electrode structure, as described above, since the arc state is a concentrated arc and the temperature is high, the wear of the contacts is accelerated, and the switching life at the time of large current interruption is shortened.

【0007】電流遮断時に発生するアークに対して、磁
界を印加する他の方法として、電極間に発生するアーク
に対して平行な軸方向の磁界を印加する方法がある。い
わゆる縦磁界電極と呼ばれているこの電極では、電極間
に発生したアークは電極全体に均一に広がり、電極の局
部的な過大な熱入力を防ぎ、遮断性能の優れた電極とす
ることができる。また、高電圧に対して電極間距離を離
したときでも、磁界の強さを適正にすることにより電極
間に安定したアークを点弧することができ、遮断性能を
上げることができる。さらに、アークの形態が電極全体
に分散したアークとなるため、大電流遮断時においても
接触子の消耗は少なく、開閉寿命を伸ばすことができ
る。
As another method of applying a magnetic field to the arc generated when the current is cut off, there is a method of applying a magnetic field in the axial direction parallel to the arc generated between the electrodes. In this so-called longitudinal magnetic field electrode, the arc generated between the electrodes spreads evenly over the entire electrode, preventing local excessive heat input of the electrode and making it an electrode with excellent blocking performance. . Further, even when the distance between the electrodes is increased with respect to the high voltage, a stable arc can be ignited between the electrodes by optimizing the strength of the magnetic field, and the breaking performance can be improved. Furthermore, since the arc form is an arc dispersed over the entire electrode, the contactor is not consumed even when a large current is interrupted, and the switching life can be extended.

【0008】ここで、軸方向磁界を発生させる従来の真
空バルブの電極構造について説明する。図4に示すよう
に、コイル電極を設け、このコイル電極に流れる電流に
より、電極間に軸方向の磁界を発生させる。このコイル
電極に流れる電流は、中心部から放射状に形成された4
本の腕部13aに分流し、各腕部13aの先端から弧状のコ
イル部13bに流れ、更に、コイル部の先端13cから接触
子に流れる。このコイル電極を可動電極側と固定電極側
の両方に取り付け、コイル部に流れる電流で軸方向の磁
界を電極間に発生させる。なお、図4では腕部13aが4
分割の場合を示したが、分割数を変えて、軸方向の磁界
の強さを変えることもできる。
Here, the electrode structure of a conventional vacuum valve for generating an axial magnetic field will be described. As shown in FIG. 4, a coil electrode is provided, and an electric field flowing in the coil electrode generates an axial magnetic field between the electrodes. The current flowing through this coil electrode is 4 formed radially from the center.
The current is divided into the arm portions 13a of the book, flows from the tip of each arm portion 13a to the arc-shaped coil portion 13b, and further flows from the tip portion 13c of the coil portion to the contact. This coil electrode is attached to both the movable electrode side and the fixed electrode side, and a magnetic field in the axial direction is generated between the electrodes by the current flowing in the coil portion. In FIG. 4, the arm portion 13a is 4
Although the case of division is shown, the strength of the magnetic field in the axial direction can be changed by changing the number of divisions.

【0009】しかしながら、このような電極構造では電
流経路が長くなって、抵抗が大きくなり、通電性能に悪
影響を及ぼす場合があった。また、抵抗を小さくするた
めには、コイル電極を厚くしたり、コイル電極の分割数
を増加させたりしたものが考えられるが、電極間に発生
する軸方向の磁界強度が減少し、十分な遮断性能が得ら
れない場合があった。さらに、構造が複雑で電極が大き
くなり、真空バルブを製作する上で、様々な問題を生
じ、信頼性を低下させる場合があった。
However, in such an electrode structure, the current path becomes long and the resistance becomes large, which may adversely affect the current-carrying performance. In order to reduce the resistance, it is conceivable to make the coil electrode thicker or increase the number of coil electrode divisions, but the magnetic field strength in the axial direction generated between the electrodes is reduced, and sufficient blocking is performed. There was a case where the performance was not obtained. Further, the structure is complicated and the electrodes are large, which causes various problems in manufacturing a vacuum valve, which may reduce reliability.

【0010】一方、より簡易な構造で軸方向の磁界を発
生させる他の電極構造として、特公平3-59531 号公報に
示されるように、カップ状の電極の円筒部分に螺旋状の
溝を形成したものがある。この電極では、円筒部の電流
経路を螺旋状にすることで、電流の弧状成分を発生さ
せ、これにより電極間に軸方向の磁界を発生させる。こ
の構成では、軸方向の磁界の強度は、円筒部の溝の傾き
を変えることで、変えることができる。
On the other hand, as another electrode structure for generating an axial magnetic field with a simpler structure, as shown in Japanese Patent Publication No. 3-59531, a spiral groove is formed in the cylindrical portion of a cup-shaped electrode. There is something I did. In this electrode, by making the current path of the cylindrical portion spiral, an arc-shaped component of the current is generated, thereby generating a magnetic field in the axial direction between the electrodes. With this configuration, the strength of the magnetic field in the axial direction can be changed by changing the inclination of the groove of the cylindrical portion.

【0011】[0011]

【発明が解決しようとする課題】しかしながら、このよ
うなカップ状電極の場合には、電極と接触子との接合部
が円筒部端面のとなり合う溝と溝の間一面に渡るため、
電流遮断時の発弧点の位置によって電極内の電流経路が
変化する。このため、発生する軸方向磁界の強度が不安
定となってしまう。例えば、図5に示すように、電流経
路が矢印Bで示される経路をとる場合には、充分な軸方
向磁界を発生できるような電流の円周方向成分を生じる
が、矢印Cで示される経路をとった場合、充分な電流の
円周方向成分を生じないので発生する軸方向磁界も弱く
なる。すなわち、遮断性能が低下することになる。本発
明の目的は、電流遮断時のアークの発弧点に関係なく、
安定して優れた遮断性能を有する真空バルブを提供する
ことにある。
However, in the case of such a cup-shaped electrode, the joint between the electrode and the contact extends over the entire surface between the grooves which are the end faces of the cylindrical portion.
The current path in the electrode changes depending on the position of the arcing point when the current is cut off. Therefore, the strength of the generated axial magnetic field becomes unstable. For example, as shown in FIG. 5, when the current path takes the path indicated by the arrow B, a circumferential component of the current that can generate a sufficient axial magnetic field is generated, but the path indicated by the arrow C. When the above is taken, a sufficient circumferential component of the electric current is not generated, so that the axial magnetic field generated is also weakened. That is, the blocking performance is reduced. The object of the present invention is, regardless of the arc firing point at the time of current interruption,
It is to provide a vacuum valve having stable and excellent shutoff performance.

【0012】[0012]

【課題を解決するための手段】上記目的を達成するため
に本発明は、真空容器内に設けられ、対向表面に接触子
を配置した接離可能な一対の電極のうち、少なくとも一
方を円筒状電極とした真空バルブにおいて、軸心に対し
て斜め方向に形成され円筒状電極の側面に設けられた複
数の溝と、円筒状電極と接触子の間に設けられた通電部
とを有し、溝と円筒状電極の接触子側端面のなす角が鋭
角である部分に通電部を備えるようにしたことを要旨と
する。
In order to achieve the above-mentioned object, the present invention is to provide at least one of a pair of electrodes which are provided in a vacuum container and which have a contactor on the opposite surface and which can be separated from each other, in a cylindrical shape. In a vacuum valve as an electrode, having a plurality of grooves formed on the side surface of the cylindrical electrode formed in a direction oblique to the axis, and a current-carrying portion provided between the cylindrical electrode and the contact, The gist is that a current-carrying portion is provided in a portion where an angle formed between the groove and the end surface of the cylindrical electrode on the contactor side is acute.

【0013】[0013]

【作用】このような構成において、円筒状電極から接触
子への電流経路は円筒状電極の側面に設けられた溝から
通電部を介して接触子へ流れる経路に定まり、電流遮断
時のアークの発弧点に関係なく、軸方向磁界を発生する
のに充分な電流円周方向成分を得ることができる。
In such a structure, the current path from the cylindrical electrode to the contactor is determined to be the path from the groove provided on the side surface of the cylindrical electrode to the contactor via the current-carrying portion, and the arc at the time of current interruption It is possible to obtain a sufficient current circumferential component for generating an axial magnetic field, regardless of the ignition point.

【0014】[0014]

【実施例】以下、本発明の一実施例を図面を参照して説
明をする。なお、電極部以外は従来のものと同一である
ため、説明を省略する。図1は本発明の一実施例を示す
真空バルブの可動電極の平面図、図2は図1の前面図で
ある。これらの図において、可動通電軸5Bの先端に可
動電極3Bが取り付けられ、この可動電極3Bの前面部
には、通電部21a,21b,21c,21dと絶縁部8a,8
b,8c,8dとから成る層が設けられ、その前面には
接触子4bが固着されている。また、このカップ状の可
動電極3Bの円筒部分には溝6a,6b,6c,6dが
形成され、底部に形成された溝7a,7b,7c,7d
と連続するように形成されている。なお、本実施例では
溝が4条の場合を示している。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. It should be noted that the description is omitted because it is the same as the conventional one except the electrode part. 1 is a plan view of a movable electrode of a vacuum valve showing an embodiment of the present invention, and FIG. 2 is a front view of FIG. In these figures, the movable electrode 3B is attached to the tip of the movable energizing shaft 5B, and the energizing portions 21a, 21b, 21c, 21d and the insulating portions 8a, 8 are provided on the front surface of the movable electrode 3B.
A layer composed of b, 8c, and 8d is provided, and a contactor 4b is fixed to the front surface thereof. Further, grooves 6a, 6b, 6c, 6d are formed in the cylindrical portion of the cup-shaped movable electrode 3B, and grooves 7a, 7b, 7c, 7d formed on the bottom are formed.
Is formed so as to be continuous with. In the present embodiment, the case where there are four grooves is shown.

【0015】電極3Bの円筒部と接触子4Bの間には溝
7a,7b,7c,7dと円筒部端面との成す角が鋭角
である側の部分に通電部21a,21b,21c,21dが設け
られ、それ以外の円筒部端面と接触子の間には絶縁部8
a,8b,8c,8dとなっている。
Between the cylindrical portion of the electrode 3B and the contactor 4B, current-carrying portions 21a, 21b, 21c and 21d are provided on the side where the angle formed by the grooves 7a, 7b, 7c and 7d and the end face of the cylindrical portion is acute. Insulating part 8 is provided between the end face of the other cylindrical part and the contactor.
a, 8b, 8c, 8d.

【0016】次に、電流の流れを説明する。電流は可動
通電軸5Bから電極底部の溝6a,6b,6c,6dに
より底部を弧状に流れて円筒部に至り、円筒部の溝7
a,7b,7c,7dおよび電極3Bと接触子4Bの間
に設けられた絶縁部8a,8b,8c,8dにより、矢
印Aのように通電部21a,21b,21c,21dを通って接
触子4Bへ流れる。これにより、電流の方向成分として
円周方向成分を生じ、軸方向磁界を発生する。そして、
接触子4Bから真空中に発生するアークを介して対向す
る固定側の接触子4Aに電流が流れ、固定電極について
も上記とほぼ同様な構造で同様な電流の流れとなる。
Next, the flow of current will be described. The electric current flows from the movable energizing shaft 5B through the grooves 6a, 6b, 6c, 6d at the bottom of the electrode in an arc shape to reach the cylindrical portion, and the groove 7 of the cylindrical portion is formed.
a, 7b, 7c, 7d and the insulating parts 8a, 8b, 8c, 8d provided between the electrode 3B and the contactor 4B, the contactor passes through the current-carrying parts 21a, 21b, 21c, 21d as shown by arrow A. It flows to 4B. As a result, a circumferential component is generated as a directional component of the current, and an axial magnetic field is generated. And
A current flows from the contactor 4B through the arc generated in the vacuum to the opposing contactor 4A on the fixed side, and the fixed electrode also has a similar structure and a similar current flow.

【0017】このように、本実施例によれば、電流経路
は溝6a〜6d,7a〜7d、絶縁8a〜8dで制限さ
れることにより、必ず通電部21a〜21dを通る。従っ
て、常に充分な円周方向成分を生じることになり、アー
クの発弧点の位置に依らず、充分な軸方向磁界を生じる
ことができ、安定で優れた遮断性能を得ることができ
る。
As described above, according to this embodiment, the current path is limited to the grooves 6a to 6d, 7a to 7d and the insulations 8a to 8d, so that the current always passes through the current-carrying portions 21a to 21d. Therefore, a sufficient circumferential component is always generated, a sufficient axial magnetic field can be generated regardless of the position of the arc ignition point, and stable and excellent breaking performance can be obtained.

【0018】なお、電極底部の溝6a,6b,6c,6
dは設けなくてもよいが、この溝を設けた方が軸方向の
磁界強度をより大きくすることができる。また、絶縁部
8a〜8dの抵抗率を通電部21a〜21dの抵抗率の40倍
以上とすれば、電流は主として電極部材を流れることに
なるので、より大きな軸方向の磁界強度を得ることがで
きる。
The grooves 6a, 6b, 6c, 6 at the bottom of the electrode
Although d may not be provided, the magnetic field strength in the axial direction can be further increased by providing this groove. Further, if the resistivity of the insulating portions 8a to 8d is 40 times or more the resistivity of the conducting portions 21a to 21d, the current mainly flows through the electrode member, so that a larger magnetic field strength in the axial direction can be obtained. it can.

【0019】本発明による真空バルブは上記実施例に限
定されるものではない。第2の実施例として、溝6a,
6b,6c,6d,7a,7b,7c,7dに抵抗率が
電極部材の40倍以上の部材、例えば電極部材が銅の場合
にはステンレス鋼を挿入するようにしてもよい。本実施
例によれば、溝に挿入された部材は電極に比べて抵抗率
が高いので電流は主として電極部材を流れることにな
り、上記実施例と同様の電流経路で軸方向磁界を発生す
ることになる。また、溝に部材を挿入するので、電極の
機械的強度を増すことができる。
The vacuum valve according to the present invention is not limited to the above embodiment. As a second embodiment, the grooves 6a,
Members 6b, 6c, 6d, 7a, 7b, 7c, and 7d whose resistivity is 40 times or more that of the electrode member, for example, stainless steel may be inserted when the electrode member is copper. According to this embodiment, since the member inserted in the groove has a higher resistivity than the electrode, the current mainly flows through the electrode member, and the axial magnetic field is generated in the same current path as in the above embodiment. become. Moreover, since the member is inserted into the groove, the mechanical strength of the electrode can be increased.

【0020】第3の実施例として、電極円筒部の接触子
側前面部の面積をSとし、溝条数をnとしたとき、接触
子と電極の間の通電部の電極円筒部接触子側前面部に占
める面積が 0.1×S/n以上1/2以下とする。通電部
をこの範囲で形成することにより、充分な遮断性能が得
られると共に、電極部分の抵抗値が小さいほど好ましい
通電性能に関し、通電部の充分な通電容量と機械的強度
を確保することができる。
As a third embodiment, assuming that the area of the contactor side front surface of the electrode cylinder is S and the number of grooves is n, the energization part between the contactor and the electrode is the electrode cylinder contactor side. The area occupying the front part should be 0.1 × S / n or more and 1/2 or less. By forming the current-carrying part in this range, sufficient breaking performance can be obtained, and sufficient current-carrying capacity and mechanical strength of the current-carrying part can be secured with respect to the current-carrying performance which is preferable as the resistance value of the electrode part is smaller. .

【0021】[0021]

【発明の効果】以上のように本発明によれば、真空容器
内に設けられ、対向表面に接触子を配置した接離可能な
一対の電極のうち、少なくとも一方を円筒状電極とした
真空バルブにおいて、軸心に対して斜め方向に形成され
円筒状電極の側面に設けられた複数の溝と、円筒状電極
と接触子の間に設けられた通電部とを有し、溝と円筒状
電極の接触子側端面のなす角が鋭角である部分に通電部
を備えるようにしたので、安定して優れた遮断性能の真
空バルブを得ることができる。
As described above, according to the present invention, a vacuum valve in which at least one of a pair of electrodes which are provided in a vacuum container and which have a contactor on the opposite surface and which can be contacted and separated is a cylindrical electrode is used. In, there are provided a plurality of grooves formed on the side surface of the cylindrical electrode diagonally with respect to the axis, and a current-carrying portion provided between the cylindrical electrode and the contact, and the groove and the cylindrical electrode. Since the current-carrying portion is provided at the portion where the contact-side end face makes an acute angle, it is possible to obtain a vacuum valve with stable and excellent breaking performance.

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

【図1】本発明の一実施例を示す真空バルブの可動電極
の平面図。
FIG. 1 is a plan view of a movable electrode of a vacuum valve showing an embodiment of the present invention.

【図2】本発明の一実施例を示す真空バルブの可動電極
の正面図。
FIG. 2 is a front view of a movable electrode of a vacuum valve showing an embodiment of the present invention.

【図3】従来の真空バルブの断面図。FIG. 3 is a sectional view of a conventional vacuum valve.

【図4】従来の真空バルブの縦磁界電極を説明するため
の図。
FIG. 4 is a diagram for explaining a vertical magnetic field electrode of a conventional vacuum valve.

【図5】従来の真空バルブの他の縦磁界電極を説明する
ための図。
FIG. 5 is a view for explaining another vertical magnetic field electrode of the conventional vacuum valve.

【符号の説明】[Explanation of symbols]

3B…可動電極、8a,8b,8c,8d…絶縁部、21
a,21b,21c,21d…通電部。
3B ... movable electrode, 8a, 8b, 8c, 8d ... insulating part, 21
a, 21b, 21c, 21d ... Current-carrying part.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 真空容器内に設けられ、対向表面に接触
子を配置した接離可能な一対の電極のうち、少なくとも
一方を円筒状電極とした真空バルブににおいて、軸心に
対して斜め方向に形成され前記円筒状電極の側面に設け
られた複数の溝と、前記円筒状電極と前記接触子の間に
設けられた通電部とを有し、前記溝と前記円筒状電極の
接触子側端面のなす角が鋭角である部分に前記通電部を
備えるようにしたことを特徴とする真空バルブ。
1. A vacuum valve having a cylindrical electrode, at least one of a pair of contactable and separable electrodes provided in a vacuum container and having a contactor disposed on an opposing surface, in a direction oblique to an axis. A plurality of grooves formed on the side surface of the cylindrical electrode and a current-carrying portion provided between the cylindrical electrode and the contactor, and the groove and the contactor side of the cylindrical electrode. A vacuum valve, wherein the energizing portion is provided in a portion where an angle formed by the end face is an acute angle.
【請求項2】 前記円筒状電極の側面に設けた複数の溝
に連続するような溝を底部に形成させるようにしたこと
を特徴とする請求項1記載の真空バルブ。
2. The vacuum valve according to claim 1, wherein a groove that is continuous with a plurality of grooves provided on the side surface of the cylindrical electrode is formed in the bottom portion.
【請求項3】 前記円筒状電極の接触子側端面の面積を
S、前記溝の条数をnとしたとき、前記通電部の前記円
筒状電極の接触子側端面に占める面積が 0.1S/n以上
1/2以下であることを特徴とする請求項1または請求
項2のいずれかに記載の真空バルブ。
3. When the area of the contact side end surface of the cylindrical electrode is S and the number of grooves of the groove is n, the area occupied by the energizing portion on the contact side end surface of the cylindrical electrode is 0.1S / It is n or more and 1/2 or less, The vacuum valve in any one of Claim 1 or Claim 2 characterized by the above-mentioned.
【請求項4】 前記円筒状電極と前記接触子の間の通電
部を除く部分の抵抗率を前記通電部の抵抗率の40倍以上
にしたことを特徴とする請求項1〜請求項3のいずれか
に記載の真空バルブ。
4. The resistivity of the portion between the cylindrical electrode and the contact excluding the current-carrying portion is set to 40 times or more the resistivity of the current-carrying portion. The vacuum valve according to any one.
【請求項5】 前記溝に前記円筒状電極部材の抵抗率の
40倍以上である抵抗率の部材を挿入するようにしたこと
を特徴とする請求項1〜請求項4のいずれかに記載の真
空バルブ。
5. The resistivity of the cylindrical electrode member is set in the groove.
The vacuum valve according to any one of claims 1 to 4, wherein a member having a resistivity of 40 times or more is inserted.
JP15775494A 1994-07-11 1994-07-11 Vacuum valve Pending JPH0822751A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15775494A JPH0822751A (en) 1994-07-11 1994-07-11 Vacuum valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15775494A JPH0822751A (en) 1994-07-11 1994-07-11 Vacuum valve

Publications (1)

Publication Number Publication Date
JPH0822751A true JPH0822751A (en) 1996-01-23

Family

ID=15656617

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15775494A Pending JPH0822751A (en) 1994-07-11 1994-07-11 Vacuum valve

Country Status (1)

Country Link
JP (1) JPH0822751A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106233414A (en) * 2014-04-17 2016-12-14 株式会社东芝 Vacuum valve

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106233414A (en) * 2014-04-17 2016-12-14 株式会社东芝 Vacuum valve
EP3133631A4 (en) * 2014-04-17 2018-01-24 Kabushiki Kaisha Toshiba Vacuum valve
US10026570B2 (en) 2014-04-17 2018-07-17 Kabushiki Kaisha Toshiba Vacuum valve
CN106233414B (en) * 2014-04-17 2019-05-31 株式会社东芝 Vacuum valve

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