JPS6065413A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS6065413A
JPS6065413A JP17217883A JP17217883A JPS6065413A JP S6065413 A JPS6065413 A JP S6065413A JP 17217883 A JP17217883 A JP 17217883A JP 17217883 A JP17217883 A JP 17217883A JP S6065413 A JPS6065413 A JP S6065413A
Authority
JP
Japan
Prior art keywords
electrode
bowl
shaped
conductor
current
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
JP17217883A
Other languages
Japanese (ja)
Inventor
森宮 脩
鈴木 節雄
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 JP17217883A priority Critical patent/JPS6065413A/en
Publication of JPS6065413A publication Critical patent/JPS6065413A/en
Pending legal-status Critical Current

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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】 〔発明の属する技術分野〕 この発明は磁場安定化形の真空遮断器に関する〔従来技
術とその問題点〕 従来の磁場安定化形の真空遮断器は、第1図に示すよう
に、少なくとも一方が可動に構成されている通電棒1と
、この通電棒1の光端に固設されている通電接点2と、
この通電接点2の外周に配置されているアーク電極3と
、このアーク電極3を通電棒Iに弾性的に保持しかっこ
の通電棒1の外周にら旋に配置した仏場発生用コイル4
とで主に構成されている。尚、これらの電極構造の図示
しない真空容器内に収納されていて、真空連断器が構成
されている。
[Detailed description of the invention] [Technical field to which the invention pertains] This invention relates to a magnetic field stabilized vacuum circuit breaker [Prior art and its problems] A conventional magnetic field stabilized vacuum circuit breaker is shown in FIG. As shown, at least one of the current-carrying rods 1 is movable, and the current-carrying contacts 2 are fixed to the light end of the current-carrying rod 1.
An arc electrode 3 is arranged around the outer periphery of the current-carrying contact 2, and a spring field generating coil 4 is arranged spirally around the outer periphery of the current-carrying rod 1, which elastically holds the arc electrode 3 on the current-carrying rod I.
It is mainly composed of. Note that these electrode structures are housed in a vacuum container (not shown) to constitute a vacuum interconnector.

このように構成されている真空遮断器の動作は、まず、
下方の通電棒1が上方に移動した状態で電気回路が導通
状態となっている。との導通状態から電気回路を遮断す
る時に1/′!、、通電棒1を下方に引き下げ通電接点
2を離間させるが、この時は接点2の表面傾接触してい
るためにコイル4に電流が流れ、コイル4の巻回方向に
応じた磁場がこれらの笈び−の周囲に発生する。この磁
iハは避Mt棒1に対して軸方向に印加されるので、電
極に生じるアーク全安定化させる作用をする。次にこの
アークを安定化した状態でさらに通電棒1を下方に移動
することにより、接点2に極部的な異常アークを生じさ
せることなく電気回路を遮断することができるのである
The operation of the vacuum circuit breaker configured in this way is as follows:
The electric circuit is in a conductive state with the lower current-carrying rod 1 moved upward. 1/' when cutting off the electrical circuit from continuity with the ,, the current-carrying rod 1 is pulled down to separate the current-carrying contacts 2, but at this time, since the surfaces of the contacts 2 are in inclined contact, a current flows through the coil 4, and a magnetic field according to the winding direction of the coil 4 is generated between them. Occurs around the kabi-. Since this magnetic flux is applied to the avoidance Mt rod 1 in the axial direction, it has the effect of completely stabilizing the arc generated at the electrode. Next, by further moving the current-carrying rod 1 downward in a state in which this arc is stabilized, the electric circuit can be interrupted without causing local abnormal arcs at the contacts 2.

しかし、アーク電極3が引き離なされる時に生じるアー
クは、電極形状と同様のドーナッツ形の中心部の畑い陽
光柱となり、安定化した遮断ができなくなる。す々わち
、このアークは力学的に不安宗で、そのドーナッツ形が
すぐに崩壊してしまい、電極−i9面の一部に片寄って
しまうのである。
However, the arc generated when the arc electrode 3 is pulled apart forms a donut-shaped central field of sunlight similar to the shape of the electrode, making stable interruption impossible. In other words, this arc is mechanically unstable, and its donut shape quickly collapses, causing it to be biased towards a part of the electrode i9 surface.

故に、真空遮断器全体として、その電極の全面を有効に
利用することができず、a場を印加し、アークを安定化
させにくい欠点があった。
Therefore, the vacuum circuit breaker as a whole has the disadvantage that the entire surface of its electrode cannot be effectively utilized, and that it is difficult to apply an a-field and stabilize the arc.

〔発明の目的〕[Purpose of the invention]

この発明は上述した従来の欠点を改良したもので、遮断
性能の安定性およびその再現性に優れかつ通電容量の大
容量化を可能とする真空遮断器を提供することを目的と
する。
The present invention improves the above-mentioned conventional drawbacks, and aims to provide a vacuum circuit breaker that has excellent stability and reproducibility of interrupting performance and can increase current carrying capacity.

〔発明の概要〕[Summary of the invention]

本発明は真空容器内に接離自在の一対の電極を有するも
のにおいて、前記電極の少なくとも一方を、他方の電極
に開口部が対面するように配置した椀状導電部と、この
椀状導電部に接続されかつ前記真空容器外に導出される
導電体と、前記椀状導体の開口部に蓋状に配置した板状
電極と、この板状電極と前記椀状導電部の底部との間に
電気的に接続しかつ弾性を有しかつ磁場を発生させるよ
う構成した磁場発生導体とを具備してなる電極構造とし
た真空遮断器であり、特に板状電極の外径を椀状4.底
部の開口部内径より小さくもしくは大きくして構成した
真空遮断器である。
The present invention has a pair of electrodes that can be freely moved into and out of contact with each other in a vacuum container, and includes a bowl-shaped conductive part in which at least one of the electrodes is arranged so that an opening faces the other electrode, and a bowl-shaped conductive part in which at least one of the electrodes is arranged so that an opening faces the other electrode. a conductor connected to and led out of the vacuum container, a plate-shaped electrode disposed in a lid-like manner at the opening of the bowl-shaped conductor, and between this plate-shaped electrode and the bottom of the bowl-shaped conductive part. It is a vacuum circuit breaker with an electrode structure comprising a magnetic field generating conductor that is electrically connected, has elasticity, and is configured to generate a magnetic field, and in particular, the outer diameter of the plate electrode is bowl-shaped. This is a vacuum circuit breaker configured to be smaller or larger than the inner diameter of the opening at the bottom.

〔発明の効果〕〔Effect of the invention〕

従来の欠点、すなわちコイル部の発熱を遮断通電の瞬時
のみとして通電容量上の間頌ヲ除去し、かつアークの安
定性を損うような電極構造上の欠点を除いた。すなわち
アーク遮断電極はほぼ平板に近く、少々くとも中心部分
の欠落(開孔部)を無くしアーク柱の根本的な不安定性
を除去するつアーク遮断電極の周辺部に椀状の通電電極
を設け、アーク安定化用磁場発生コイル要素を椀状電極
の四部に設けこのコイル要素の一方を椀状電極の底部あ
るいわ周辺部に接続し、他方を椀状電極の開孔部に蓋状
に設けた遮断電極に接続する。投入時は椀状通電電極に
よりコイル要素両端が短絡されるのでコイルの発熱を防
ぐことができ、大容量通電が可能となった。
The drawbacks of the conventional method, namely, the generation of heat in the coil section only at the moment of interruption and energization, have been eliminated, and the drawbacks of the current carrying capacity have been eliminated, as well as the drawbacks of the electrode structure that impair the stability of the arc. In other words, the arc-breaking electrode is almost a flat plate, and a bowl-shaped current-carrying electrode is provided around the periphery of the arc-breaking electrode to at least eliminate the lack of a hole in the center (hole) and eliminate the fundamental instability of the arc column. , magnetic field generating coil elements for arc stabilization are provided in four parts of the bowl-shaped electrode, one of these coil elements is connected to the bottom or periphery of the bowl-shaped electrode, and the other is provided in the opening of the bowl-shaped electrode in the shape of a lid. Connect to the cut-off electrode. When the coil is turned on, both ends of the coil element are short-circuited by the bowl-shaped current-carrying electrode, which prevents heat generation in the coil and enables large-capacity current flow.

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

以下、本発明の実症例について詳に(dに説明する。 Hereinafter, an actual case of the present invention will be explained in detail in (d).

本発明のべ空遮断器は例えば圧力が10 Pa以下に排
気されている真空容器(図示せず)内に接離自在の一対
の電極構造を収納してNpされている。この6空容器に
収納されている電極構造は、第2図に示すように、一方
(下側)が可動、可能に他方(上側)が固定されている
一対の椀状導電部5と、この椀状2#電部5の開口縁部
に設けたリング状の通電電極6と、椀状導電部5の開口
部7に蓋をするように配置した板状の遮断電極8と、こ
の遮断電極8と椀状導電部の底部9との間を電気的に接
続すると共に弾性を有するコイル状の磁場発生導体10
と。
The air circuit breaker of the present invention is constructed by housing a pair of electrode structures that can be freely moved into and out of contact with each other in a vacuum container (not shown) which is evacuated to a pressure of 10 Pa or less, for example. As shown in Fig. 2, the electrode structure housed in these six empty containers consists of a pair of bowl-shaped conductive parts 5, one of which (lower side) is movable and the other (upper side) of which is fixed. A ring-shaped current-carrying electrode 6 provided at the edge of the opening of the bowl-shaped 2# conductive part 5, a plate-shaped cut-off electrode 8 arranged to cover the opening 7 of the bowl-shaped conductive part 5, and this cut-off electrode. 8 and the bottom part 9 of the bowl-shaped conductive part, and a coil-shaped magnetic field generating conductor 10 having elasticity.
and.

椀状導電部9を真空容器外に導出する導電$11と、遮
断電極8に貼設した補強用導電体12と、椀状導電部9
の外周囲に増設した補強体13とでEIEに眉1!成さ
れている。
A conductor 11 that leads the bowl-shaped conductive part 9 out of the vacuum container, a reinforcing conductor 12 attached to the cutoff electrode 8, and a bowl-shaped conductive part 9.
With reinforcement body 13 added around the outer circumference, EIE has 1 eyebrow! has been completed.

このように榊欣、された本発明の真空遮11斤¥袴の動
作は次のように行なわれている。まず4電棒11を上昇
させて投入した時には、回路電流カニ〕市電導体6を介
して椀状導体5を辿り真空容ン器の夕を部回路に流入出
するが、コイル導体10はl’6tf椀状専体椀状短体
5れているのでこの電流は流第1−J’l コイルの間
熱はない。遮断時は、導電棒11を下方に抄年下させる
ことにより行なわれるが、その降下過4呈に吃いて、ま
ず初めに通電電極6が開離しその表m1にアークが発生
する。しかしこの時点では遮断1狂極8はまた接触して
いるので、回路電流は上方の通電棒11→コイル導体1
0→補強用導電体12→遮断電極8→下方の遮断電接8
→補強用導電体12→コイル導体10→通電棒11の順
に主電流が流れ、通電電極間には電流が流れ外くなるの
で通電電極の表面に生じていたアークは消滅する。次に
さらに通電棒11が下降すると遮断電極8が開離し、こ
んどけ給断電極面にアークが発生する。このアークは磁
場発生要素であるコイル導体1oによって生じた安定化
磁場(軸方向磁場)の作用によって電極の全面にほぼ均
一に分布して発生する。このように安定化されたアーク
はさらに導電棒11が下降すると電流零点をもって遮断
される。故に、コイル導体1゜が加熱されることなく、
電極間に発生するアークを安定させて回路遮断ができる
ので、真空遮断器としての性能が向」:する。
The operation of the vacuum-shielded 11 loin yen hakama of the present invention, which has been made as described above, is carried out as follows. First, when the four electric rods 11 are raised and turned on, the circuit current follows the bowl-shaped conductor 5 via the city electric conductor 6, and flows into and out of the vacuum container into the circuit, but the coil conductor 10 is l'6tf. Since there is a bowl-shaped short body 5, this current flows and there is no heat between the coils. When the conductive rod 11 is cut off, it is carried out by lowering the conductive rod 11 downward, but as the rod 11 falls, the current-carrying electrode 6 first separates and an arc is generated on its surface m1. However, at this point, the cutoff 1 crazy pole 8 is in contact again, so the circuit current flows from the upper current-carrying rod 11 to the coil conductor 1.
0 → Reinforcing conductor 12 → Breaking electrode 8 → Lower breaking electrical connection 8
The main current flows in the order of → reinforcing conductor 12 → coil conductor 10 → current-carrying rod 11, and since the current flows between the current-carrying electrodes and disconnects them, the arc that has been generated on the surface of the current-carrying electrodes disappears. Next, when the current carrying rod 11 is further lowered, the cutoff electrode 8 is separated, and an arc is generated on the surface of the supply and cutoff electrode. This arc is generated in a substantially uniform distribution over the entire surface of the electrode due to the action of a stabilizing magnetic field (axial magnetic field) generated by the coil conductor 1o, which is a magnetic field generating element. The arc stabilized in this way is cut off at the current zero point when the conductive rod 11 is further lowered. Therefore, 1° of the coil conductor is not heated,
The circuit can be broken by stabilizing the arc generated between the electrodes, improving its performance as a vacuum circuit breaker.

〔発明の他の実施例〕[Other embodiments of the invention]

次に本発明の他の実施例について説明する。尚、同一構
成部分については同一符号を附して説明する。・第3図
に示す電極構造は、前述同様に図示しない真空容器に収
納されている。椀状導体5の開口部7にはその開口部7
を、間隙14を有して覆うように、板状の遮断電極15
がコイル導体10に設けられている。すなわち、この遮
断電極15は、その外径が椀状導体5の内径より大きく
形成されている。ただし、実用的にその外径は椀状導体
5の外径と同一径となっているが大きくとも小さくとも
良いが、少なくとも内径より大きければ良い。また、こ
の遮断電極15は同一部材で作っても良いが、第3図に
示すように補強導電体16に貼着しても良い。椀状導体
5の通電電極6とはこれと対向する位僅にリング状の接
触電極17を補強2!%電体16の周囲に設けて電気的
に接続する。
Next, other embodiments of the present invention will be described. Note that the same components will be described with the same reference numerals. - The electrode structure shown in FIG. 3 is housed in a vacuum container (not shown) as described above. The opening 7 of the bowl-shaped conductor 5 has its opening 7
A plate-shaped cutoff electrode 15 is placed so as to cover with a gap 14.
is provided on the coil conductor 10. That is, this cutoff electrode 15 is formed so that its outer diameter is larger than the inner diameter of the bowl-shaped conductor 5. However, for practical purposes, its outer diameter is the same as the outer diameter of the bowl-shaped conductor 5, but it may be larger or smaller, as long as it is at least larger than the inner diameter. The cutoff electrode 15 may be made of the same material, or may be attached to a reinforcing conductor 16 as shown in FIG. Reinforce the ring-shaped contact electrode 17 slightly opposite the current-carrying electrode 6 of the bowl-shaped conductor 5! It is provided around the electric body 16 and electrically connected to it.

このように構成された真空遮断器は次のように動作する
。投入時は電流は通電を通し外部より導入され、椀状導
体5を通電、通電接点6、遮断電極15、通電接点6、
椀状導体5を通り、対向する他方の通電棒11を通り外
部へ流出する。このとき磁場発生要素であるコイル導体
10はほぼ短絡された状態とり、コイル導体10にはほ
とんど電流が流れないので発熱は起らない。
The vacuum circuit breaker constructed in this manner operates as follows. At the time of turning on, the current is passed through and introduced from the outside, and the bowl-shaped conductor 5 is energized, the current-carrying contact 6, the cutoff electrode 15, the current-carrying contact 6,
It passes through the bowl-shaped conductor 5, passes through the other opposing current-carrying rod 11, and flows out to the outside. At this time, the coil conductor 10, which is a magnetic field generating element, is in a substantially short-circuited state, and almost no current flows through the coil conductor 10, so no heat is generated.

遮断時は先ず通電電極6が開離しアークが発生する。し
かし遮断?l’1−t15はまだ接勉しているので、電
流はコイル導体10fK:介して流れ、通電型’jFf
i6と遮断11¥極15の接点17間に生じたアークは
直ちに消滅する。次に遮断電極15が開離しアークが発
生するっこのアークは磁場発生要素10によって生ずる
安定化磁場(軸方向磁場)によシ安定化され電極15の
全面にほぼ均一に分布する。この電(セ2間に生じたア
ークは電流零点t−まらて遮断される。尚、第2図と第
3図とに示した実施例の相異は、第2図に示した方では
通電電極の接触部と遮断型(砂の接触部とは並列に接続
されて−いるのに反し、第3図では二つの通電接触部と
遮断電極の接触部とが直列に接続されている点である。
At the time of interruption, the current-carrying electrode 6 is first separated and an arc is generated. But blocking? Since l'1-t15 is still in close contact, the current flows through the coil conductor 10fK:, and the energizing type 'jFf
The arc generated between i6 and the contact 17 of the cutoff 11\pole 15 is immediately extinguished. Next, the interrupting electrode 15 opens and an arc is generated. This arc is stabilized by the stabilizing magnetic field (axial magnetic field) generated by the magnetic field generating element 10 and is distributed almost uniformly over the entire surface of the electrode 15. The arc generated between this electric current and the current zero point t is interrupted.The difference between the embodiments shown in FIGS. 2 and 3 is that the one shown in FIG. In contrast to the contact part of the current-carrying electrode and the contact part of the breaking type (sand), which are connected in parallel, in Figure 3, the two current-carrying contact parts and the contact part of the breaking electrode are connected in series. It is.

尚、上述した各々の実施例では一つの電極に一つの磁場
発生要素(コイル導体)を示したが、二つ以上の磁場発
生要素(コイル導体)を並列に接続しても効果は変らな
い。またコイル導体の構造は円筒コイル状となっている
が平面状のコイルでも効果は変らない。
In each of the embodiments described above, one magnetic field generating element (coil conductor) is shown for one electrode, but the effect does not change even if two or more magnetic field generating elements (coil conductor) are connected in parallel. The structure of the coil conductor is a cylindrical coil, but the effect is the same even if it is a planar coil.

磁場発生用コイル導体の材質は賃温に加熱Jれても弾性
を失わないステンレス綱、インコネル等が良い。また通
電容量(遮断瞬時の)を増すために前記弾性材と銅のよ
うな導電材との複合材料を用いても良い。
The material of the magnetic field generating coil conductor is preferably stainless steel, Inconel, etc., which do not lose their elasticity even when heated to low temperatures. Furthermore, a composite material of the elastic material and a conductive material such as copper may be used to increase the current carrying capacity (instantly when the current is interrupted).

椀状通電導体5.あるいは遮断電極8,15はいずれも
単一金属に限らずステンレス綱等からなる適当な補強部
材12,13.16e設けても良い。
Bowl-shaped current-carrying conductor 5. Alternatively, the cutoff electrodes 8 and 15 are not limited to being made of a single metal, but may be provided with suitable reinforcing members 12, 13, 16e made of stainless steel or the like.

また遮断電極8,15あるいは通電棒11には磁束の短
絡効果を低減させるために適当な切溝(図示していない
)を設けることが望ましい。
Further, it is desirable to provide appropriate grooves (not shown) in the cutoff electrodes 8, 15 or the current-carrying rod 11 in order to reduce the short-circuiting effect of magnetic flux.

また発生磁場の分布、強度の増加等のため適当な材質、
形状の強磁性体18を設けても本発明の作用効果は損わ
れない。
In addition, suitable materials are used to increase the distribution and strength of the generated magnetic field.
Even if the shaped ferromagnetic body 18 is provided, the effects of the present invention are not impaired.

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

第1図は従来の真空遮断器の一部を示す断面図、第2図
は本発明にかかわる真空遮断器の要部を示す断面図、第
3図は本発明の他の実施例の要部を示す断面図である。 5・・椀状導体、6・・・通電電極、8・・・遮断電極
、10・・ 場発生用装置(コイル導体)、11・・通
電棒。 第 1 図 第2図 第 3 図
FIG. 1 is a sectional view showing a part of a conventional vacuum circuit breaker, FIG. 2 is a sectional view showing a main part of a vacuum circuit breaker according to the present invention, and FIG. 3 is a main part of another embodiment of the present invention. FIG. 5... Bowl-shaped conductor, 6... Current-carrying electrode, 8... Cutting-off electrode, 10... Field generation device (coil conductor), 11... Current-carrying rod. Figure 1 Figure 2 Figure 3

Claims (3)

【特許請求の範囲】[Claims] (1) A空容器内に接離自在の一対の電極を有するも
のにおいて、前記電極の少なくとも一方を、他方の電極
に開口部が対面するように配置した 状導覗部と、この
椀状導電部に接続されかつ前記真空容器外に導出される
導電体と、前記椀状導体の開口部に蓋状に配置した板状
電極と、この板状電極と前記椀状導電部の底部との間に
電気的に接続しかつ弾性を有しかつ前記椀状導電部が他
方の接点に接触しない範囲で磁場を発生させるよう構成
した磁場発生導体とを具備してなる電極構造としたこと
を特徴とする真空遮断器。
(1) In a device having a pair of electrodes that can be freely brought into contact and separated from each other in an empty container A, at least one of the electrodes is arranged such that the opening faces the other electrode, and the bowl-shaped conductive part a conductor connected to the conductor and led out of the vacuum vessel; a plate-shaped electrode disposed in a lid-like manner at the opening of the bowl-shaped conductor; and between this plate-shaped electrode and the bottom of the bowl-shaped conductor. and a magnetic field generating conductor that is electrically connected to the contact point, has elasticity, and is configured to generate a magnetic field within a range where the bowl-shaped conductive part does not come into contact with the other contact. Vacuum circuit breaker.
(2)板状電極の外径を椀状導電部の開口部内径より小
さくしたことを特徴とする特許請求の範囲第1項記載の
真空遮断器。
(2) The vacuum circuit breaker according to claim 1, wherein the outer diameter of the plate electrode is smaller than the inner diameter of the opening of the bowl-shaped conductive part.
(3)板状?l?、極の外径を椀状導電部の開口部内径
より大きくしたことを特徴とする特許請求の範囲第1項
記載の真空遮断器。
(3) Platy? l? 2. The vacuum circuit breaker according to claim 1, wherein the outer diameter of the pole is larger than the inner diameter of the opening of the bowl-shaped conductive part.
JP17217883A 1983-09-20 1983-09-20 Vacuum breaker Pending JPS6065413A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17217883A JPS6065413A (en) 1983-09-20 1983-09-20 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17217883A JPS6065413A (en) 1983-09-20 1983-09-20 Vacuum breaker

Publications (1)

Publication Number Publication Date
JPS6065413A true JPS6065413A (en) 1985-04-15

Family

ID=15937017

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17217883A Pending JPS6065413A (en) 1983-09-20 1983-09-20 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS6065413A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011104751A1 (en) * 2010-02-24 2011-09-01 三菱電機株式会社 Vacuum valve
JP2014099417A (en) * 2007-06-05 2014-05-29 Cooper Technologies Co Vacuum interrupter
JP2015519713A (en) * 2012-06-11 2015-07-09 アーベーベー テクノロジー アクチエンゲゼルシャフトABB Technology AG Vacuum circuit breaker with double coaxial contact configuration on both sides

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014099417A (en) * 2007-06-05 2014-05-29 Cooper Technologies Co Vacuum interrupter
WO2011104751A1 (en) * 2010-02-24 2011-09-01 三菱電機株式会社 Vacuum valve
JP5281192B2 (en) * 2010-02-24 2013-09-04 三菱電機株式会社 Vacuum valve
JP2015519713A (en) * 2012-06-11 2015-07-09 アーベーベー テクノロジー アクチエンゲゼルシャフトABB Technology AG Vacuum circuit breaker with double coaxial contact configuration on both sides

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