JPH07220588A - Vacuum valve - Google Patents

Vacuum valve

Info

Publication number
JPH07220588A
JPH07220588A JP1020794A JP1020794A JPH07220588A JP H07220588 A JPH07220588 A JP H07220588A JP 1020794 A JP1020794 A JP 1020794A JP 1020794 A JP1020794 A JP 1020794A JP H07220588 A JPH07220588 A JP H07220588A
Authority
JP
Japan
Prior art keywords
electrode
current
magnetic field
vacuum valve
electrodes
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
JP1020794A
Other languages
Japanese (ja)
Inventor
Kiyobumi Otobe
清文 乙部
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 JP1020794A priority Critical patent/JPH07220588A/en
Publication of JPH07220588A publication Critical patent/JPH07220588A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To provide a vacuum valve having excellent current-carrying performance and disconnection performance. CONSTITUTION:A coil electrode has an electrode base 8, and an arc part provided along an outer form of the electrode base 8, and current-carrying members 7a-7d having connection parts 7a2-7d2 to be connected to the electrode base 8 are disposed like a ring. The adjacent current-carrying members, that is 7a and 7d, for example, are disposed to face each other in the axial direction of the electrode having a specified gap between each other.

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】遮断時にアークに平行な磁界を発生させ
るコイル電極を用いた真空バルブの電極部分の代表的な
構成図を図5に示す。同図において、電極1は、主電極
2と、その背面に設けられたコイル電極3と、主電極2
とコイル電極3との間に設けられた補強部材4から構成
されている。ここで、コイル電極3は、通電軸5に固着
される中央接続部3aと、中央接続部3aから外周に向
かって延びている腕部3bと、その先端から通電軸5と
同心で円弧状に延びて電流経路を形成する外周円弧部3
cと、主電極2に電気的に接続する接続突起部3dが設
けられている。このような構成において、各外周円弧部
3cを流れる円周方向の電流に基づいて対向する電極間
にアークに平行な磁界(以下、軸方向磁界と記す。)を
発生させ、電極間に生ずる真空アークを安定化して大電
流の遮断を可能にしている。
2. Description of the Related Art FIG. 5 shows a typical constitution of an electrode portion of a vacuum valve using a coil electrode for generating a magnetic field parallel to an arc when breaking. In the figure, an electrode 1 includes a main electrode 2, a coil electrode 3 provided on the back surface thereof, and a main electrode 2
The reinforcing member 4 is provided between the coil electrode 3 and the coil electrode 3. Here, the coil electrode 3 has a central connecting portion 3a fixed to the energizing shaft 5, an arm portion 3b extending from the central connecting portion 3a toward the outer periphery, and a circular arc shape concentric with the energizing shaft 5 from its tip. Circumferential arc portion 3 extending to form a current path
c and a connecting protrusion 3d for electrically connecting to the main electrode 2 are provided. In such a configuration, a magnetic field parallel to the arc (hereinafter referred to as an axial magnetic field) is generated between the electrodes facing each other based on the current in the circumferential direction flowing through each outer circumferential arc portion 3c, and the vacuum generated between the electrodes. It stabilizes the arc and makes it possible to interrupt large currents.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、このよ
うな真空バルブの電極1の構成においては、電流経路は
通電軸5からコイル電極3の中央接続部3a−腕部3b
−外周円弧部3c−接続突起部3dを通って主電極2に
至る経路となる。一方、一対の電極間ギャップの中間部
に発生する磁界の強度分布は、図6に示すように、電極
の中心軸上が最大になり、周辺に向かって次第に減少す
る分布となる。ここで、磁界の分布が縦方向に幅を持つ
のは円周方向の変動によるものである。
However, in such a structure of the electrode 1 of the vacuum valve, the current path is from the current-carrying shaft 5 to the central connecting portion 3a of the coil electrode 3 to the arm portion 3b.
-Outer peripheral circular arc portion 3c-It becomes a path to the main electrode 2 through the connecting projection portion 3d. On the other hand, as shown in FIG. 6, the intensity distribution of the magnetic field generated in the intermediate portion of the gap between the pair of electrodes is the maximum on the central axis of the electrode and gradually decreases toward the periphery. Here, the distribution of the magnetic field has a width in the vertical direction due to the fluctuation in the circumferential direction.

【0004】また、コイル電極3の外周円弧部3c上の
磁界分布を円周方向の角度に対してプロットすると図7
のようになる。この場合は、図5の電極に対応した磁界
分布を示しており、コイルの腕部が4つに分かれている
ことから一方の電極の腕部を基準に0度から90度までを
表示している。残りの90度から360 度までの磁界分布は
この繰り返しである。このような磁界強度の変動は、電
流経路の中で接続突起部3dと腕部3bとの間のギャッ
プ部は電流が流れないので円弧状の電流が完全なリング
を形成していないこと、および腕部3bに流れる電流の
影響があることの2つの原因で発生する。
Further, when the magnetic field distribution on the outer circumferential arc portion 3c of the coil electrode 3 is plotted against the angle in the circumferential direction, FIG.
become that way. In this case, the magnetic field distribution corresponding to the electrodes in FIG. 5 is shown. Since the arm portion of the coil is divided into four, the arm portion of one electrode is used as a reference and 0 to 90 degrees are displayed. There is. The remaining magnetic field distribution from 90 to 360 degrees repeats this. Such a variation in the magnetic field strength is caused by the fact that the arc-shaped current does not form a perfect ring because no current flows in the gap between the connection protrusion 3d and the arm 3b in the current path. It occurs due to two causes of the influence of the current flowing through the arm portion 3b.

【0005】この磁界強度の変動の幅は、対向する電極
の円周方向の位置関係によっても変わる。磁界強度の強
弱の分布によって、電流遮断能力に影響がでてくること
が知られており、電流遮断時に電極間に発生するアーク
を安定に維持するために、一般的には磁界強度の分布は
変動の少ないことが望ましい。また、安定した遮断性能
を得るためには、磁界分布が常に同じ状態で真空バルブ
が製作されることが望ましいが、従来の電極例では、相
対する一対の電極の円周方向の位置を管理して製作する
必要があり、製造工程上の位置管理や部品による位置決
め等による部品費および製造費の増大を招く。
The width of the fluctuation of the magnetic field strength also changes depending on the positional relationship in the circumferential direction of the opposing electrodes. It is known that the distribution of the strength of the magnetic field affects the current interruption capability.In order to maintain the arc generated between the electrodes during current interruption stable, the distribution of the magnetic field strength is generally It is desirable that there is little fluctuation. Also, in order to obtain stable cutoff performance, it is desirable to manufacture a vacuum valve with the magnetic field distribution always the same, but in the conventional electrode example, the position of the pair of electrodes facing each other in the circumferential direction is controlled. It is necessary to manufacture it by the above-mentioned method, which causes an increase in parts cost and manufacturing cost due to position management in the manufacturing process and positioning by parts.

【0006】そのうえ、このような電極では、通電容量
の増大を遮断性能の低下を招くことなく達成することが
難しい。通電容量を増大させる方法の1つにコイル電極
3の外周円弧部3cや腕部3dの通電断面積を大きくし
て通電抵抗を小さくすることが考えられるが、外周円弧
部3cを流れる円弧方向の電流が電極間から遠ざかるこ
とになり、電極間に発生する磁界強度の減少を招く。ま
た、円弧方向の電流の半径が小さくなることにより軸方
向磁界の有効面積が減少する。いずれも遮断性能の低下
を招く要因となる。
Moreover, with such an electrode, it is difficult to increase the current-carrying capacity without lowering the breaking performance. One possible method of increasing the current carrying capacity is to increase the current carrying cross-sectional area of the outer circumferential arc portion 3c of the coil electrode 3 or the arm portion 3d to reduce the current carrying resistance. The electric current is moved away from between the electrodes, which causes a decrease in the magnetic field strength generated between the electrodes. In addition, the effective area of the axial magnetic field decreases due to the smaller radius of the current in the arc direction. Any of these causes a reduction in the blocking performance.

【0007】また、通電容量を増大させる他の方法とし
て、コイル電極3の腕の数を増やすことが考えられる
が、円弧状の電流値が腕の数に反比例して減少すると共
に、隣り合った腕の隙間の部分が多くなり、円弧状の電
流の欠落により磁界強度が減少し、遮断性能が低下す
る。本発明の目的は、通電性能および遮断性能に優れた
真空バルブを提供することにある。
As another method of increasing the current carrying capacity, it is conceivable to increase the number of arms of the coil electrode 3, but the arc-shaped current value decreases in inverse proportion to the number of arms, and the adjacent electrodes are adjacent to each other. The gaps in the arms increase, and the lack of arc-shaped current reduces the magnetic field strength, which lowers the breaking performance. An object of the present invention is to provide a vacuum valve excellent in energization performance and interruption performance.

【0008】[0008]

【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、真空容器と、真空容器に接離自在に配設さ
れた一対の電極と、一対の電極の少なくとも一方の背部
に接続され、電極間に軸方向磁界を発生させるコイル電
極とを備えた真空バルブにおいて、コイル電極は、電極
台と、電極台の外形に沿った円弧部を持ち、一端が電極
台に接続される複数の通電子とを有し、通電子をリング
状に配置し、隣接する通電子を所定の間隙を有しながら
電極の軸方向に対向させるようにしたことを特徴とす
る。
In order to achieve the above object, the present invention is directed to a vacuum container, a pair of electrodes arranged so as to come in contact with and separate from the vacuum container, and a back portion of at least one of the pair of electrodes. In the vacuum valve provided with a coil electrode for generating an axial magnetic field between the electrodes, the coil electrode has an electrode base and an arc portion along the outer shape of the electrode base, and one end of which is connected to the electrode base. And the adjacent ones are arranged so as to face each other in the axial direction of the electrode while having a predetermined gap.

【0009】[0009]

【作用】このような構成において、複数の通電子をリン
グ状に配置し、隣接する通電子を電極の軸方向に重なり
合うようにしたので、円弧成分の電流を部分的に途切ら
せることなく流すことができ、磁界強度の減少を防ぐこ
とができる。
In such a structure, a plurality of conduction electrons are arranged in a ring shape and adjacent conduction electrons are overlapped with each other in the axial direction of the electrode, so that the current of the arc component flows without being partially interrupted. It is possible to prevent the magnetic field strength from decreasing.

【0010】[0010]

【実施例】以下、本発明の一実施例を図面を参照して詳
細に説明する。ただし、従来のものと同一のものについ
ては同一番号を付して説明を省略する。図1は本発明の
真空バルブの電極部分の側面図、図2は図1の一方の分
解斜視図、図3は図2の通電子7aの構成図である。こ
れらの図において、2は主電極、6はコイル電極、7a
〜7dは通電子、5は通電軸、8は電極台、9は補強部
材であり、コイル電極6は通電子7a〜7dと電極台8
を有する。通電子7a〜7dは電極台8の外周に沿った
円弧状に形成され、両端に接続部7a1〜7d1および
7a2〜7d2を設けてあり、それぞれ主電極2および
電極台8に接続される。また、通電軸5は電極台8に接
続され、電極台8と主電極2の間は補強部材9が挿入接
続されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below in detail with reference to the drawings. However, the same parts as the conventional ones are designated by the same reference numerals and the description thereof will be omitted. FIG. 1 is a side view of an electrode portion of a vacuum valve of the present invention, FIG. 2 is one exploded perspective view of FIG. 1, and FIG. 3 is a configuration diagram of a conduction member 7a of FIG. In these figures, 2 is a main electrode, 6 is a coil electrode, and 7a.
7d is a conducting electron, 5 is a current-carrying shaft, 8 is an electrode base, 9 is a reinforcing member, and the coil electrode 6 is a conducting member 7a to 7d and an electrode base 8.
Have. The conducting electrons 7a to 7d are formed in an arc shape along the outer periphery of the electrode base 8, and have connecting portions 7a1 to 7d1 and 7a2 to 7d2 at both ends, which are connected to the main electrode 2 and the electrode base 8, respectively. The energizing shaft 5 is connected to the electrode base 8, and the reinforcing member 9 is inserted and connected between the electrode base 8 and the main electrode 2.

【0011】一方、通電子7aは、両端に設けた接続部
7a1,7a2と、上部円弧部7a3、下部円弧部7a
4とからなる。下部円弧部7a4の上部には、隣接する
通電子7dの上部円弧部7d3が、上部円弧部7a3の
下部には隣接する通電子7bの下部円弧部7b4が所定
のギャップを設けて対向配置されている。その他の通電
子間も同様である。
On the other hand, the conducting member 7a has connecting portions 7a1 and 7a2 provided at both ends, an upper arc portion 7a3, and a lower arc portion 7a.
4 and. The upper arc portion 7d3 of the adjacent conduction electron 7d is disposed above the lower arc portion 7a4, and the lower arc portion 7b4 of the adjacent conduction electron 7b is disposed below the upper arc portion 7a3 so as to face each other with a predetermined gap. There is. The same applies to other communication devices.

【0012】このような構成において、通電軸5から電
極台8を通って流れる電流は、各通電子7a〜7dへ分
流し軸方向磁界を発生させる円弧成分の電流となり、主
電極2へ流入する。ここで、通電子7a〜7dは互いに
隣接する通電子と重なり合うようにして対向配置される
ので、円弧状の電流成分が部分的に途切れることはな
い。また、通電子の重なり合う部分があることにより電
流経路が1ターン以上となり、従来のコイル電極による
電流経路の場合より大きなターン数が得られ、磁界強度
の増大が図れる。
In such a structure, the current flowing from the current-carrying shaft 5 through the electrode base 8 is a current of an arc component that divides the current into the current-carrying electrons 7a to 7d to generate an axial magnetic field, and flows into the main electrode 2. . Here, since the conduction electrons 7a to 7d are arranged to face each other so as to overlap the conduction electrons adjacent to each other, the arc-shaped current component is not partially interrupted. Further, the current path has one or more turns due to the overlapping portions of the conduction electrons, so that a larger number of turns can be obtained and the magnetic field strength can be increased as compared with the current path using the conventional coil electrode.

【0013】以上のように本実施例によれば、軸方向磁
界を発生させる電流の円弧成分が部分的に途切れること
がないので、図4に示すように、円周方向の強度の変動
が少ない均一な磁界分布が得られる。また、電流の円弧
成分のターン数を従来の縦磁界電極に比べ大きくできる
ので磁界強度を増大できる。したがって、遮断性能の向
上がはかれる。
As described above, according to the present embodiment, the arc component of the electric current for generating the axial magnetic field is not partially interrupted, so that the fluctuation of the intensity in the circumferential direction is small as shown in FIG. A uniform magnetic field distribution can be obtained. Further, since the number of turns of the arc component of the current can be made larger than that of the conventional longitudinal magnetic field electrode, the magnetic field strength can be increased. Therefore, the breaking performance can be improved.

【0014】また、通電容量の増大を図るためにコイル
電極の通電子の通電断面積を大きくして通電抵抗を小さ
くした場合でも、従来の縦磁界電極に比べターン数が大
きいことから必要な軸方向磁界強度が得られ易く、遮断
性能の低下を招くことなく通電容量を増大することが容
易である。さらに、本実施例では、各通電子7a〜7d
は図3からわかるように短い経路を取ることができない
ようになっているため、隣り合う腕部が上下に重なり合
うようにでき、磁界分布の不均一を招くことがなく、遮
断性能を低下させることがない。
Even when the conduction cross section of the conduction of the coil electrode is increased to reduce the conduction resistance in order to increase the conduction capacity, the required number of turns is larger than that of the conventional longitudinal magnetic field electrode. Directional magnetic field strength is easily obtained, and it is easy to increase the current-carrying capacity without lowering the breaking performance. Further, in the present embodiment, each of the communication electrons 7a to 7d.
As can be seen from FIG. 3, it is not possible to take a short path, so that adjacent arm parts can be made to overlap vertically, which does not cause non-uniformity of the magnetic field distribution and lowers the breaking performance. There is no.

【0015】なお、本発明は本実施例に限られることな
く、例えば、通電子の数は2個以上であればよい。ま
た、通電子は上部円弧部、下部円弧部、および接続部を
それぞれ別個に構成し接続してもよいし、上部円弧部と
下部円弧部間に段部を設けずに傾斜状に構成してもよ
い。
The present invention is not limited to this embodiment, and the number of conducting electrons may be two or more, for example. Further, in the conduction electron, the upper circular arc portion, the lower circular arc portion, and the connecting portion may be separately configured and connected, or may be formed in an inclined shape without providing a step portion between the upper circular arc portion and the lower circular arc portion. Good.

【0016】さらに、本実施例のように、各通電子をギ
ャップを介して絶縁するのではなく、絶縁物を介した
り、通電子表面に絶縁物をコーティングしたものでもよ
い。ギャップを介する場合でも、ギャップを維持するた
めに種々の補強を設けてもよい。
Further, as in the present embodiment, instead of insulating the respective conduction electrons through the gaps, it is also possible to use an insulation or coat the conduction surface with an insulation. Various reinforcements may be provided to maintain the gap even through the gap.

【0017】一方、電極台8に軸方向磁界の交流電流に
よる変動で発生する渦電流の発生を防止するために、半
径方向にスリットを設けると、より一層の性能向上が図
れる。
On the other hand, if a slit is provided in the radial direction on the electrode base 8 in order to prevent the generation of an eddy current caused by the fluctuation of the axial magnetic field due to the alternating current, the performance can be further improved.

【0018】[0018]

【発明の効果】以上のように本発明によれば、真空容器
と、真空容器に接離自在に配設された一対の電極と、一
対の電極の少なくとも一方の背部に接続され、電極間に
軸方向磁界を発生させるコイル電極とを備えた真空バル
ブにおいて、コイル電極は、電極台と、電極台の外形に
沿った円弧部を持ち、一端が電極台に接続される複数の
通電子とを有し、通電子をリング状に配置し、隣接する
通電子を所定の間隙を有しながら電極の軸方向に対向さ
せるようにしたので、通電性能および遮断性能に優れた
真空バルブを得ることができる。
As described above, according to the present invention, the vacuum container, the pair of electrodes disposed so as to come in contact with and separate from the vacuum container, and the back of at least one of the pair of electrodes are connected to each other, and between the electrodes. In a vacuum valve including a coil electrode that generates an axial magnetic field, the coil electrode includes an electrode base and a plurality of electrons having an arc portion along the outer shape of the electrode base and one end of which is connected to the electrode base. Since the energizing electrons are arranged in a ring shape and the adjoining energizing electrons are opposed to each other in the axial direction of the electrode with a predetermined gap, it is possible to obtain a vacuum valve having excellent energizing performance and interruption performance. it can.

【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電極部分
の側面図。
FIG. 1 is a side view of an electrode portion of a vacuum valve showing an embodiment of the present invention.

【図2】〔図1〕の分解斜視図。FIG. 2 is an exploded perspective view of FIG.

【図3】〔図2〕の通電子7aの斜視図。FIG. 3 is a perspective view of a conduction electron 7a of FIG. 2;

【図4】〔図1〕の真空バルブの電極部分により発生す
る磁界の強度分布を示す図。
FIG. 4 is a diagram showing an intensity distribution of a magnetic field generated by an electrode portion of the vacuum valve of FIG.

【図5】代表的な真空バルブの電極部分の分解斜視図。FIG. 5 is an exploded perspective view of an electrode portion of a typical vacuum valve.

【図6】〔図5〕の真空バルブの電極部分により発生す
る磁界の強度分布を説明するための図。
FIG. 6 is a diagram for explaining the intensity distribution of a magnetic field generated by the electrode portion of the vacuum valve of FIG. 5;

【図7】〔図5〕の真空バルブの電極部分により発生す
る磁界の強度分布を説明するための図。
FIG. 7 is a diagram for explaining the intensity distribution of a magnetic field generated by the electrode portion of the vacuum valve of FIG.

【符号の説明】[Explanation of symbols]

2…主電極、6…コイル電極、7a〜7d…通電子、8
…電極台。
2 ... Main electrode, 6 ... Coil electrode, 7a-7d ... Electron, 8
… Electrode stand.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 真空容器と、この真空容器に接離自在に
配設された一対の電極と、この一対の電極の少なくとも
一方の背部に接続され、前記電極間に軸方向磁界を発生
させるコイル電極とを備えた真空バルブにおいて、前記
コイル電極は、電極台と、この電極台の外形に沿った円
弧部を持ち、一端が前記電極台に接続される複数の通電
子とを有し、前記通電子をリング状に配置し、隣接する
通電子を所定の間隙を有しながら前記電極の軸方向に対
向させるようにしたことを特徴とする真空バルブ。
1. A coil which is connected to a vacuum container, a pair of electrodes arranged so as to be able to come into contact with and separated from the vacuum container, and at least a back part of the pair of electrodes, and which generates an axial magnetic field between the electrodes. In a vacuum valve provided with an electrode, the coil electrode has an electrode base and a plurality of electrons having an arc portion along the outer shape of the electrode base and having one end connected to the electrode base. A vacuum valve characterized in that conducting electrons are arranged in a ring shape, and adjacent conducting electrons are opposed to each other in the axial direction of the electrode with a predetermined gap.
【請求項2】 前記コイル電極の電極台に、前記電極の
半径方向のスリットを設けたことを特徴とする請求項1
記載の真空バルブ。
2. The electrode base of the coil electrode is provided with a slit in the radial direction of the electrode.
Vacuum valve as described.
JP1020794A 1994-02-01 1994-02-01 Vacuum valve Pending JPH07220588A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1020794A JPH07220588A (en) 1994-02-01 1994-02-01 Vacuum valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1020794A JPH07220588A (en) 1994-02-01 1994-02-01 Vacuum valve

Publications (1)

Publication Number Publication Date
JPH07220588A true JPH07220588A (en) 1995-08-18

Family

ID=11743833

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1020794A Pending JPH07220588A (en) 1994-02-01 1994-02-01 Vacuum valve

Country Status (1)

Country Link
JP (1) JPH07220588A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104465204A (en) * 2013-09-12 2015-03-25 Ls产电株式会社 Electrode assembly and vacuum interrupter including the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104465204A (en) * 2013-09-12 2015-03-25 Ls产电株式会社 Electrode assembly and vacuum interrupter including the same

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