JPH06139886A - Vacuum valve - Google Patents

Vacuum valve

Info

Publication number
JPH06139886A
JPH06139886A JP28840692A JP28840692A JPH06139886A JP H06139886 A JPH06139886 A JP H06139886A JP 28840692 A JP28840692 A JP 28840692A JP 28840692 A JP28840692 A JP 28840692A JP H06139886 A JPH06139886 A JP H06139886A
Authority
JP
Japan
Prior art keywords
electrode
contact
vacuum valve
electrodes
melting point
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
JP28840692A
Other languages
Japanese (ja)
Inventor
Kenji Watanabe
憲治 渡辺
Eiji Kaneko
英治 金子
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 JP28840692A priority Critical patent/JPH06139886A/en
Publication of JPH06139886A publication Critical patent/JPH06139886A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To provide a vacuum valve increasing the critical current value at an electrode to form an arc spot when the current is cut off and maintaining the excellent cutoff performance. CONSTITUTION:Contact pieces 7 at the middle section and outer periphery of a contact 5 are formed into a protruded shape toward an electrode 4 side on the contact 5 of the electrode 4 of a vacuum valve. The material of a recessed contact piece 8 at the middle section has the melting point, heat conductivity, specific heat, and density larger than those of the material of the contact piece 7.

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係り、特に
電極構造に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a vacuum valve, and more particularly to an electrode structure.

【0002】[0002]

【従来の技術】遮断電流を向上させるための真空バルブ
の電極構造として、真空アークに平行な磁界を印加する
縦磁界形電極がある。縦磁界形の構造にもいくつかある
が、ここでは、図3に示した構造のものについて説明す
る。
2. Description of the Related Art As an electrode structure of a vacuum valve for improving a breaking current, there is a vertical magnetic field type electrode for applying a magnetic field parallel to a vacuum arc. Although there are some vertical magnetic field type structures, the structure shown in FIG. 3 will be described here.

【0003】図3に示した真空バルブの固定及び可動電
極は同軸上に配置され、可動側の通電軸は図示しない操
作機構部にベローズを介して接続される。構造的には、
可動及び固定側電極同一であり、電極間の中心線に対し
て対称な構造になっている。以下、一方の電極について
説明していく。
The fixed and movable electrodes of the vacuum valve shown in FIG. 3 are arranged coaxially, and the movable current-carrying shaft is connected to an operation mechanism portion (not shown) via a bellows. Structurally,
The movable and fixed electrodes are the same, and the structure is symmetrical with respect to the center line between the electrodes. Hereinafter, one of the electrodes will be described.

【0004】通電軸1を流れる電流は、コイル電極2の
腕部を通じて半径方向に流れ、さらに電極円周方向に設
けられた電流通路を流れることにより軸方向の磁界を発
生させることができる。さらに、この電流は接続子3、
電極4、接点5に流れる。
A current flowing through the current-carrying shaft 1 flows in a radial direction through the arm portion of the coil electrode 2 and further flows in a current passage provided in the circumferential direction of the electrode to generate a magnetic field in the axial direction. Furthermore, this current is
It flows to the electrode 4 and the contact 5.

【0005】一方、電流遮断時には、電極4間にアーク
が点弧され、可動及び固定電極は電気的に接続されてい
ることになり、電流は対向する電極に向かって前述した
逆の順番で流れる。
On the other hand, when the current is cut off, an arc is ignited between the electrodes 4, the movable and fixed electrodes are electrically connected, and the current flows toward the opposing electrodes in the reverse order described above. .

【0006】ところで、アークに平行な磁界を印加する
ことによって、アークを電極面全体に一様に広げること
ができることはよく知られている。従って、このような
電極構造にしたことにより大電流領域までアノードスポ
ット(遮断時に悪影響を及ぼす)の形成を抑制すること
ができる。またアノード電極の一部が過度に過熱され、
電流遮断時でもアノード電極の表面温度がかなり高いの
で電極材料の蒸発が盛んとなり、遮断不能に至るのを防
いでいる。
By the way, it is well known that the arc can be uniformly spread over the entire electrode surface by applying a magnetic field parallel to the arc. Therefore, with such an electrode structure, it is possible to suppress the formation of an anode spot (which has an adverse effect upon interruption) up to a large current region. Also, part of the anode electrode is overheated,
Even when the electric current is cut off, the surface temperature of the anode electrode is considerably high, so that the evaporation of the electrode material becomes active and the interruption of the electric current is prevented.

【0007】[0007]

【発明が解決しようとする課題】しかしながら、従来の
真空バルブの電極構造では、使用する接点材料、電極径
によりアノードスポットの形成される臨界電流値が一義
的に決まってしまう。この臨界電流値を大きくするた
め、縦磁界強度及び分布の最適化を図った電極構造にす
る必要があり、その調整が極めて難しい。また、このよ
うな調整をしても臨界電流値を十分に大きくできるとは
言い難い。
However, in the conventional vacuum valve electrode structure, the critical current value at which the anode spot is formed is uniquely determined by the contact material used and the electrode diameter. In order to increase this critical current value, it is necessary to have an electrode structure that optimizes the longitudinal magnetic field strength and distribution, and its adjustment is extremely difficult. Further, it is hard to say that the critical current value can be made sufficiently large even with such adjustment.

【0008】本発明の目的は、同一電極径であってもア
ノードスポットが形成される臨界電流値を大きくでき、
優れた遮断性能を維持できる真空バルブを提供すること
にある。
The object of the present invention is to increase the critical current value at which the anode spot is formed even if the electrode diameter is the same,
It is to provide a vacuum valve that can maintain excellent shutoff performance.

【0009】[0009]

【課題を解決するための手段および作用】上記目的を達
成するために本発明は、真空容器内に一対の電極が接離
可能に設けられ、一対の電極に電極の軸方向と平行な磁
界を発生する電極を備えた真空バルブにおいて、一対の
電極の接点の中心部および外周部は中間部よりも対向電
極側に凸状に設けられ、接点の中間部は中心部および外
周部よりも融点、熱伝導率、比熱、および密度が大きい
材料としたので、アノードスポットが形成される臨界電
流値を大きくすることができる。
In order to achieve the above object, according to the present invention, a pair of electrodes are provided in a vacuum container so that they can come into contact with and separate from each other, and a magnetic field parallel to the axial direction of the electrodes is applied to the pair of electrodes. In a vacuum valve provided with an electrode for generating, a central portion and an outer peripheral portion of contact points of a pair of electrodes are provided in a convex shape on the counter electrode side with respect to an intermediate portion, and an intermediate portion of the contact point has a melting point higher than the central portion and the outer peripheral portion, Since the material having large thermal conductivity, specific heat and density is used, the critical current value for forming the anode spot can be increased.

【0010】[0010]

【実施例】以下、本発明の実施例を図面を参照して説明
する。なお従来と同様のものについては、同一番号を付
して説明を省略する。
Embodiments of the present invention will be described below with reference to the drawings. The same parts as those of the conventional one are designated by the same reference numerals and the description thereof will be omitted.

【0011】図1は本発明の真空バルブの電極の断面図
である。同図において、電極4の接点の中心部および外
周部を対向する他の電極側へ凸状に形成される接触子7
とし、これらの間にある中間部は接触子8として示され
るように接触子7からみてくぼむようになる。
FIG. 1 is a sectional view of an electrode of a vacuum valve of the present invention. In the same figure, the contactor 7 is formed so that the central portion and the outer peripheral portion of the contact point of the electrode 4 project toward the other facing electrode
The intermediate portion between them becomes concave as seen from the contactor 7, as shown by the contactor 8.

【0012】さらに詳細に説明すれば、融点が高く、密
度・比熱・熱伝導率の大きい接触子8(例えば、モリブ
デン、タングステンから成る)の表面が接触子7の表面
より数mm低くするために、電極中心と外周の中間領域
にリング状にザグリを設けている。このリング状領域の
半径方向の長さは、電極半径の10〜20%程度でよい。
More specifically, in order to make the surface of the contact 8 (made of, for example, molybdenum or tungsten) having a high melting point and a large density, specific heat and thermal conductivity lower than the surface of the contact 7 by several mm. A ring-shaped counterbore is provided in the intermediate region between the electrode center and the outer periphery. The radial length of the ring-shaped region may be about 10 to 20% of the electrode radius.

【0013】一方、電極4上の中心部及び外周部には、
高耐圧・大電流遮断用の接触子7(例えば、Cu−Cr
から成る)を電極4とろう付けしている。また、電極4
のリング状ザグリ部の上には融点が高く、密度・比熱・
熱伝導率の大きい接触子Bをろう付けしている。電流遮
断時においては、可動または固定電極のいずれもアノー
ド側になる可能性があるので、両方ともこのような電極
構造にしている。
On the other hand, in the central portion and the outer peripheral portion on the electrode 4,
Contact 7 for breaking high voltage and large current (eg Cu-Cr
(Comprising) is brazed to the electrode 4. Also, the electrode 4
The melting point is high on the ring-shaped counterbore part of
The contactor B having a large thermal conductivity is brazed. When the current is cut off, either the movable electrode or the fixed electrode may be on the anode side, so both electrodes have such an electrode structure.

【0014】本発明者がこのような電極構造を見出した
のは次のような知見に基づいたからである。すなわち、
アノードスポットが形成されるまでを説明する一般論
は、大電流領域において、アノード近傍での電流分布が
収縮し、アノードの一部に過大な入力エネルギー(アノ
ード電極に到達する電子・イオン等によるエネルギー)
があり、電極表面が融点に達して電極からの材料の蒸発
が盛んとなるからと考えられている。従って、アノード
スポットの形成を大電流まで抑制するには、入力エネル
ギーの集中を抑えるか、または入力エネルギーが入射し
ても表面が融点に達しないようにすることである。縦磁
界は前者に対して有効ではあるが後者に対しては有効と
いえないので、後者のように改善を図る必要があった。
図2に縦磁界を印加された電極の温度分布を示した特性
図である。
The present inventor has found such an electrode structure based on the following knowledge. That is,
The general theory to explain the formation of the anode spot is that in a large current region, the current distribution near the anode contracts, causing excessive input energy (energy due to electrons, ions, etc. reaching the anode electrode) to a part of the anode. )
It is considered that the electrode surface reaches the melting point and the evaporation of the material from the electrode becomes active. Therefore, in order to suppress the formation of the anode spot up to a large current, it is necessary to suppress the concentration of the input energy or prevent the surface from reaching the melting point even when the input energy is incident. The longitudinal magnetic field is effective for the former but not effective for the latter, so it is necessary to improve it like the latter.
FIG. 2 is a characteristic diagram showing a temperature distribution of an electrode to which a vertical magnetic field is applied.

【0015】同図によれば、電極中心部と外周部の間の
中間部で最も熱入力が大きくなる(最高温度になる)こ
とがわかる。このため、図1に示したように、最も熱入
力が大きい領域に融点が高く、密度・比熱・熱伝導率の
大きい接触子8を埋設しておくことにより、熱入力が大
きくても材料の融点にアーク期間中達することが従来よ
りかなり抑制される。従って、接触子Aのみを使用した
場合にくらべアノードスポットが形成される臨界電流値
を大幅に向上させる。
According to the figure, it can be seen that the heat input becomes maximum (maximum temperature) at the intermediate portion between the electrode central portion and the outer peripheral portion. Therefore, as shown in FIG. 1, by embedding the contact 8 having a high melting point and a high density, specific heat, and high thermal conductivity in a region having the largest heat input, even if the heat input is large, Reaching the melting point during the arc period is considerably suppressed compared to the past. Therefore, the critical current value at which the anode spot is formed is significantly improved as compared with the case where only the contact A is used.

【0016】また、一方の電極はカソード側になるが、
接触子8の表面が接触子7の表面より数mm下がってい
るので、カソードスポットが接触子8には点弧し難しく
なる。従って、電極間に形成されるアークプラズマはほ
とんどが接触子Aから蒸発したものとなり、接触子8の
影響が極力抑えられる。このため、アノード電極に入力
されるエネルギーは、従来とほとんど変わらないものと
なると考えられる。
One electrode is on the cathode side,
Since the surface of the contactor 8 is lower than the surface of the contactor 7 by several mm, the cathode spot is ignited on the contactor 8 and becomes difficult. Therefore, most of the arc plasma formed between the electrodes is evaporated from the contactor A, and the influence of the contactor 8 can be suppressed as much as possible. Therefore, it is considered that the energy input to the anode electrode will be almost the same as the conventional one.

【0017】[0017]

【発明の効果】以上のように本発明によれば、真空容器
内の一対の電極の接点を、その中心部および外周部は中
間部よりも対向する電極側へ凸状に設けるとともに、中
間部は中心部および外周部よりも融点・熱伝導率・比熱
・密度を大きい材料としたので使用する接点材料、電極
径に関係なく電極におけるアークスポットが形成される
臨界電流値を大きくでき、優れた遮断性能を維持できる
真空バルブを得ることができる。
As described above, according to the present invention, the contact points of the pair of electrodes in the vacuum container are provided so that the central portion and the outer peripheral portion thereof are convex toward the opposing electrode side rather than the intermediate portion, and the intermediate portion is formed. Is a material whose melting point, thermal conductivity, specific heat and density are higher than those of the central and outer parts, so the critical current value at which an arc spot is formed on the electrode can be increased regardless of the contact material used and the electrode diameter. It is possible to obtain a vacuum valve that can maintain the shutoff performance.

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

【図1】本発明の真空バルブの電極部分の断面図。FIG. 1 is a sectional view of an electrode portion of a vacuum valve of the present invention.

【図2】一般的な縦磁界電極を有する真空バルブの電極
の温度分布を示す図。
FIG. 2 is a diagram showing a temperature distribution of electrodes of a vacuum valve having a general longitudinal magnetic field electrode.

【図3】従来の真空バルブの電極部分の断面図。FIG. 3 is a sectional view of an electrode portion of a conventional vacuum valve.

【符号の説明】[Explanation of symbols]

4…電極、5…接点、7,8…接触子 4 ... Electrode, 5 ... Contact, 7, 8 ... Contact

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 真空容器内に一対の電極が接離可能に設
けられ、この一対の電極に電極の軸方向と平行な磁界を
発生する電極を備えた真空バルブにおいて、前記一対の
電極の接点の中心部および外周部は中間部よりも対向電
極側に凸状に設けられ、前記接点の中間部は中心部およ
び外周部よりも融点、熱伝導率、比熱、および密度が大
きい材料としたことを特徴とする真空バルブ。
1. A vacuum valve in which a pair of electrodes are provided in a vacuum container so that they can come into contact with and separate from each other, and the pair of electrodes has an electrode for generating a magnetic field parallel to the axial direction of the electrodes. The central portion and outer peripheral portion of the contact point are provided in a convex shape on the counter electrode side with respect to the intermediate portion, and the intermediate portion of the contact is made of a material having a higher melting point, thermal conductivity, specific heat, and density than the central portion and outer peripheral portion. Vacuum valve characterized by.
JP28840692A 1992-10-27 1992-10-27 Vacuum valve Pending JPH06139886A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28840692A JPH06139886A (en) 1992-10-27 1992-10-27 Vacuum valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28840692A JPH06139886A (en) 1992-10-27 1992-10-27 Vacuum valve

Publications (1)

Publication Number Publication Date
JPH06139886A true JPH06139886A (en) 1994-05-20

Family

ID=17729801

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28840692A Pending JPH06139886A (en) 1992-10-27 1992-10-27 Vacuum valve

Country Status (1)

Country Link
JP (1) JPH06139886A (en)

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