JPS58129718A - Vacuum interrupter - Google Patents

Vacuum interrupter

Info

Publication number
JPS58129718A
JPS58129718A JP1267582A JP1267582A JPS58129718A JP S58129718 A JPS58129718 A JP S58129718A JP 1267582 A JP1267582 A JP 1267582A JP 1267582 A JP1267582 A JP 1267582A JP S58129718 A JPS58129718 A JP S58129718A
Authority
JP
Japan
Prior art keywords
magnetic field
electrode
cylindrical
intermediate lead
lead body
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
JP1267582A
Other languages
Japanese (ja)
Inventor
佐野 孝光
横山 寿輝
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.)
Meidensha Corp
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Corp
Meidensha Electric Manufacturing Co Ltd
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 Meidensha Corp, Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Corp
Priority to JP1267582A priority Critical patent/JPS58129718A/en
Publication of JPS58129718A publication Critical patent/JPS58129718A/en
Pending legal-status Critical Current

Links

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】 本発明は真空インタラプタに係シ、特にアークに対し平
行な軸方向磁界を発生させる手段を電極の背部に備えて
なる真空インタラプタに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to vacuum interrupters, and more particularly to a vacuum interrupter comprising means behind the electrodes for generating an axial magnetic field parallel to the arc.

近年、アークにこれと平行な軸方向の磁界を印加するこ
とによシ、アークを電極面上に分散せしめてその局部的
な集中を防止し、もって電極の過度の溶融を防止するこ
とによりしゃ断能力の向上を図った、いわゆる縦磁界方
式(アーク分散方式)の真空インタラゲタが知られてい
る。
In recent years, by applying an axial magnetic field parallel to the arc, it is possible to disperse the arc on the electrode surface and prevent its local concentration, thereby preventing excessive melting of the electrode. A so-called vertical magnetic field type (arc dispersion type) vacuum interrogator with improved performance is known.

かかる縦磁界方式の真空インタラプタは、真空容器内に
その軸線上に位置せしめて相対的に接近離反自在に導入
した1対の電極棒を介し対をなす電極を接触離反(接t
ili6 )自在に設けるとともに、各市(ヴとそれぞ
れの電極棒の内端部とを、電極の背部に配設されかつ電
極棒に流れる電流を電極棒を中心とするループ電流に変
更して軸方向の磁界を発生させるコイル(磁界発生体)
により電気的に接続して構成されるのが一般的である。
Such a vertical magnetic field type vacuum interrupter brings a pair of electrodes into contact with and away from each other through a pair of electrode rods that are positioned on the axis of the vacuum container and introduced so that they can move toward and away from each other.
ili6) At the same time, each city (V) and the inner end of each electrode rod are arranged at the back of the electrode, and the current flowing through the electrode rod is changed to a loop current centered on the electrode rod, and the axial direction A coil that generates a magnetic field (magnetic field generator)
Generally, it is configured to be electrically connected to each other.

かかる縦磁界方式の真空インタラプタにおいてその通電
電流容量をあげるには、コイルを分流タイプのものとす
ればよいが、コイルの分割数に反比例して軸方向磁界の
強度が低下し、しゃ断能力が低下するという問題がある
。この問題に対処するには、電極をたとえばステンレス
鋼により形成した場合において大電流をしゃ断するのに
最適な軸方向磁界は、その磁束密度が40〜60G/K
Aであることが実験により確かめられ、またステンレス
鋼の電極および嗜等のコイルの外径を100m+*とす
るとともに、電極間ギャップおよびコイルの分割数を変
化せしめた場合における軸方向磁界の磁束密度の計算値
および抑j定結果を表わした次表からも判るように、 分割数0の1ターンまたは分割数2のlAターンのコイ
ルを用いればよいことが知られている。
In order to increase the carrying current capacity of such a vertical magnetic field type vacuum interrupter, it is possible to use a shunt type coil, but the strength of the axial magnetic field decreases in inverse proportion to the number of divisions of the coil, and the breaking ability decreases. There is a problem with doing so. To deal with this problem, the optimal axial magnetic field for cutting off large currents when the electrodes are made of stainless steel, for example, has a magnetic flux density of 40 to 60 G/K.
It has been confirmed by experiment that A is the case, and the magnetic flux density of the axial magnetic field when the outer diameter of the stainless steel electrode and the coil is 100 m+*, and the gap between the electrodes and the number of divisions of the coil are changed. As can be seen from the following table showing the calculated value of and the result of suppression, it is known that it is sufficient to use a 1 turn coil with a division number of 0 or a 1A turn coil with a division number of 2.

ところが、縦磁界方式の真空インタラプタのコイル等は
、従来、第1図2g2図に示すように1髪けられていた
。すなわち、第1図において1は電袷俸で、図示しない
真空容器に導入される内端部には、第2図に示すように
、円板状の取付部2aと、この取付部2aの外周におけ
る対称位置から半径方向(第1図、第2図において左右
方向)外方へ延伸した2個の腕部2bと、各腕部2bの
端部から相隣る腕部2bの端部方向へ同一の方向性4の
一方を介して嵌着されているとともに、笠形円板状の電
極5が、その背面(第1図において下面)中央部に凹設
した四部6とコイル2における取付部2aの他方の凹部
4とに両端を嵌着した截頭円錐体状の電極絶縁支持体7
を介し直列的に固着されている。そして、コイル2と電
極5とは、コイル2における各磁界発生部2Cの端部の
孔8に一端を嵌着するとともに他端を電極5の背面周辺
に接合した軸方向(第1図において上下方向)の通電ビ
ン9を介し電気的に接続されているものである。
However, the coils and the like of vertical magnetic field type vacuum interrupters have conventionally been cut off by one hair, as shown in Fig. 1, 2g and 2. That is, in FIG. 1, reference numeral 1 denotes an electric conductor, and as shown in FIG. Two arm portions 2b extend outward in the radial direction (horizontal direction in FIGS. 1 and 2) from symmetrical positions, and from the end of each arm portion 2b toward the end of the adjacent arm portion 2b. The cap-shaped disk-shaped electrode 5 is fitted through one side of the same directionality 4, and is recessed in the center of the back (lower surface in FIG. 1) of the fourth part 6 and the attachment part 2a of the coil 2. a truncated cone-shaped electrode insulating support 7 whose both ends are fitted into the other recess 4;
They are fixed in series through. The coil 2 and the electrode 5 are connected in the axial direction (up and down in FIG. It is electrically connected via the current-carrying bottle 9 in the direction (direction).

なお、電極絶縁支持体7は、電極棒1と電極5とが電気
的に直接に接続されるのを防止して電極5を電極棒1に
支持するためのもので、ステンレス鋼の如き高電気抵抗
の金属またはセラミックスの如き電気絶縁物からなるも
のである。また、第1図において10はコイル2を補強
支持するコイル補強体で、ステンレス鋼等からなるもの
である。
The electrode insulating support 7 is for supporting the electrode 5 on the electrode rod 1 while preventing the electrode rod 1 and the electrode 5 from being directly electrically connected. It is made of electrically insulating materials such as resistive metals or ceramics. Further, in FIG. 1, reference numeral 10 denotes a coil reinforcing body for reinforcing and supporting the coil 2, and is made of stainless steel or the like.

しかるに、上述した従来のコイル等は、磁界発生部が円
周方向において2分割されているため、半径方向の腕部
を必要とし、その機械的強度の低下および軸方向磁界の
損失を招来し、また通電ピンを介して電極と接続される
ので、通電容量の不足に伴う発熱等のためにその使用に
耐え得ないという問題がある。
However, in the conventional coils and the like described above, the magnetic field generating section is divided into two in the circumferential direction, and therefore requires a radial arm section, resulting in a decrease in mechanical strength and a loss of the axial magnetic field. Furthermore, since it is connected to the electrode via a current carrying pin, there is a problem that it cannot withstand use due to heat generation due to insufficient current carrying capacity.

本発明は、上述した問題に鑑みてなされたもので、その
目的とするところは、磁界発生部を径方向へ同心状に分
割するとともに、各磁界発生部を唯:極に設けた円筒部
および電極棒に固着した中間リード体の円筒部を介し電
極および電極棒と電気的に接続することによシ、大容量
の電流を通電し得るとともに、優れたしゃ断性能でしゃ
断し得るようにした縦磁界方式の真空インタラプタを提
供するにある。以下、第3図以降の図面を参照してこの
発明の実施例を詳細に説、明する。
The present invention has been made in view of the above-mentioned problems, and its purpose is to divide the magnetic field generating part concentrically in the radial direction, and to form a cylindrical part in which each magnetic field generating part is provided as a pole. By electrically connecting the electrode and the electrode rod through the cylindrical part of the intermediate lead body fixed to the electrode rod, a vertical conductor that can conduct a large amount of current and cut off with excellent cutting performance. To provide a magnetic field type vacuum interrupter. Hereinafter, embodiments of the present invention will be described and explained in detail with reference to the drawings from FIG. 3 onwards.

本発明に係る真空インタラプタは、第3図に示すように
、円柱状の真空容器11内にその軸線上に位置せしめて
1対の電極棒12を相対的に接近離反自在に導入し、各
771極棒12の内端部に大容量の電流を投入、しゃ断
すべく接離される対をなす笠形円板状の電極13を電気
絶縁性支持部材を介在せしめて直列的に固着するととも
に、各電極棒12とそれぞれの電極13とを電極13の
背部に配設されかつ電極棒12に流れる軸方向(第3図
において上下方向)の通電電流fc電極棒12を中心と
するループ電流に変更して軸方向磁界を発生させるコイ
ル14によりトχ続して概略構成されている。
As shown in FIG. 3, the vacuum interrupter according to the present invention has a pair of electrode rods 12 positioned on the axis of a cylindrical vacuum container 11 and introduced so as to be able to approach and separate from each other. A pair of cap-shaped disk-shaped electrodes 13 that are brought into contact and separated in order to input and cut off a large amount of current to the inner end of the pole rod 12 are fixed in series with an electrically insulating support member interposed, and each electrode The rod 12 and each electrode 13 are arranged at the back of the electrode 13, and the axial current (vertical direction in FIG. 3) flowing through the electrode rod 12 is changed to fc, a loop current centered around the electrode rod 12. It is generally constructed of a coil 14 that generates an axial magnetic field.

すなわち、真空容器11は、円筒状に成形したガラスま
たはアルミナ質のセラミックスからなる複数(本実施例
においては2個)の絶縁筒15を、それぞれの両端に気
密接続したコバールの如き金属材料からなる薄肉円筒状
の封着金具16 、16゜・・・の一方を介して1本の
絶縁筒とするとともに、その両開口端を他方の封着金具
16.16を介し円板状の金属端板17,17によシ気
密に封止し、かつ内部を高真空に排気して形成されてい
る。そして、真空容器11内には、前記対をなす電極棒
12が各金属端板17の中央に設けた孔17aから真空
容器11の気密性を保持して相対的に接近離反自在に導
入きれている。
That is, the vacuum container 11 is made of a metal material such as Kovar, which has a plurality (two in this embodiment) of insulating cylinders 15 formed into a cylindrical shape made of glass or alumina ceramics and hermetically connected to both ends of each insulating cylinder 15. One of the thin cylindrical sealing fittings 16, 16°... is connected to form a single insulating cylinder, and both open ends are connected to the other sealing fitting 16, 16 to form a disc-shaped metal end plate. 17, 17 are hermetically sealed and the inside is evacuated to a high vacuum. The pair of electrode rods 12 are introduced into the vacuum container 11 through holes 17a provided in the center of each metal end plate 17 so as to be able to approach and separate from each other while maintaining the airtightness of the vacuum container 11. There is.

なお、一方(第3図において上方)の電極棒12は、一
方の金属端板17に気密に接合されているものであり、
他方の電極棒12は、金属ベローズ18により真空容器
11の気密性を保持しつつ他方の金属端板17の孔17
aを軸方向へ移動自在に挿通されるとともに、真空容器
11の外部に配設される図示しない操作装置を介し往復
駆動されるものである。また、第3図において19は電
極13.18等を同心状に囲繞する円筒状の主シールド
で、その中間部付近を前記一方の封着金具16に挾持さ
れたリング円板状の支持金具2oにより支持されるもの
であJ、21.21は各金属端板17の内面に固着した
補助シールドである1、前記他方(可動側)の電極棒1
2の内端部には、第4図に示すように、前記コイル14
の一部を構成する中間リード体22が、電極13の外径
とほぼ同径の円板状に形成した取付部22aの一面中央
に凹設した凹部23を介し嵌合されかつろう付けにより
固着されている。取付部22aの他面には、その外径と
同径の第1円筒部22bおよび電極棒12とほぼ同外径
の第2円筒部22cが同心状に一体成形されており、各
円筒部22b、22cの対向する内周面および外周面に
は、後述する磁界発生体の嵌着を容易にすべく段部24
,25が形成されている。中間リード体22は、後述す
る如く径方向(第3図、第4図において左右方向)の同
一平面内において同心状に配設される磁界発生体と電極
棒12とを電気的に接続するためのものであり、電極棒
12の内端部付近に嵌着したリング円板状にしてかつオ
ーステナイト系ステンレス鋼の如く機械的強度の大きい
金属からなる補強金具26により、その取付部22aの
一面をろう付は接合されて補強支持されている。中間リ
ード体22の取付部22aの他面における第2円筒部2
2cに囲繞された部分には、両端にフランジ部27a 
、27bを一体成形したオーステナイト系ステンレス鋼
の如き高電気抵抗の金属またはセラミックスの如き電気
絶縁物からなる円筒状の電極絶縁支持部材27が、先端
の7ランジ部27aを各円筒部22b、22cの開口端
より突出せしめて基端のフランジ部27bを介し嵌合さ
れかつろう付けにより固着されている。
Note that one (upper in FIG. 3) electrode rod 12 is hermetically joined to one metal end plate 17.
The other electrode rod 12 is connected to the hole 17 of the other metal end plate 17 while maintaining the airtightness of the vacuum container 11 with the metal bellows 18.
It is inserted through the tube so as to be freely movable in the axial direction, and is driven back and forth via an operating device (not shown) disposed outside the vacuum container 11. In FIG. 3, reference numeral 19 denotes a cylindrical main shield concentrically surrounding the electrodes 13, 18, etc., and a ring disk-shaped support fitting 2o is sandwiched near the middle part by the one sealing fitting 16. J, 21 is an auxiliary shield fixed to the inner surface of each metal end plate 17, and the other (movable side) electrode rod 1 is supported by J.
At the inner end of the coil 14, as shown in FIG.
The intermediate lead body 22 constituting a part of the electrode 13 is fitted through a recess 23 recessed in the center of one surface of the mounting portion 22a, which is formed in a disk shape with approximately the same diameter as the outer diameter of the electrode 13, and is fixed by brazing. has been done. A first cylindrical portion 22b having the same outer diameter as the mounting portion 22a and a second cylindrical portion 22c having approximately the same outer diameter as the electrode rod 12 are integrally molded concentrically on the other surface of the mounting portion 22a. , 22c are provided with a stepped portion 24 on the opposing inner and outer peripheral surfaces in order to facilitate the fitting of a magnetic field generator, which will be described later.
, 25 are formed. The intermediate lead body 22 is used to electrically connect the magnetic field generating body and the electrode rod 12, which are arranged concentrically in the same plane in the radial direction (the left-right direction in FIGS. 3 and 4), as described later. One surface of the mounting portion 22a is secured by a reinforcing fitting 26 that is shaped like a ring disk and is made of a metal with high mechanical strength such as austenitic stainless steel, which is fitted near the inner end of the electrode rod 12. Brazing is joined and reinforced. The second cylindrical portion 2 on the other surface of the attachment portion 22a of the intermediate lead body 22
The portion surrounded by 2c has flange portions 27a at both ends.
A cylindrical electrode insulating support member 27 made of a high electrical resistance metal such as austenitic stainless steel or an electrical insulator such as ceramics is integrally molded with 7 flange portions 27a at the tip of each cylindrical portion 22b, 22c. It protrudes from the opening end, is fitted through the flange portion 27b at the base end, and is fixed by brazing.

前記電極絶縁支持部材27には、中間リード体22の第
1円筒m22 bと第2円筒部22cとのほぼ中間の外
径を有する円筒部18aを背面(第4図において下面)
に一体成形した前記電極13が、その円筒部13aを中
間リード体22の各円筒部22b、22cと半径方向に
おいて交互に重畳せしめるとともに、その背面中央部に
凹設した凹部28を先端のフランジ部27aに嵌合しか
つろう付けして固着されている。そして、中間り一ド体
22の第1円筒部22bと電極13の円筒部13a並び
に電極13の円筒部18aと中間リード体22の第2円
筒部22cとは、それぞれ中間リード体22と相俟って
前記コイル14を構成する第1磁界発生体29並びに第
2磁界発生体30によシミ見向に接続されている。第1
磁界発生体29および第2磁界発生体30は、通電電流
の経路を電極棒12を中心とするループ状に変更して軸
方向磁界を発生させるもので、第4図、第6図に示すよ
うに、中間リード体22の第1円筒部22bの内周面お
よび電極18の円筒部18aの内周面と嵌合してろう付
けにより固着される外リング部29aおよび30aと、
電極13の円筒部13aの外周面および中間リード体2
2の第2円筒部22Cの外周面と嵌合してろう付けによ
り固着される内リング部29 bおよび30bと、それ
ぞれの外リング部29aおよび30aと内リング部29
1)および30bとの間を通7!j:’l流が矢印で示
すように同一円周方向へ流れるようにlii[すべく両
リング部の中間の外径を有する有端環状にしてかつ両端
に半径方向の接続部を備えた1個の磁界発生部29cお
よび80cとからなり、各部の断面が軸方向へ長い長矩
形状に設けられるとともに、各部が一体成形されている
ものである。
The electrode insulating support member 27 has a cylindrical portion 18a having an outer diameter approximately intermediate between the first cylinder m22b and the second cylindrical portion 22c of the intermediate lead body 22 on the back (lower surface in FIG. 4).
The cylindrical portion 13a of the electrode 13 is integrally formed with the cylindrical portions 22b and 22c of the intermediate lead body 22 in the radial direction, and a recess 28 formed in the center of the back surface is formed in the flange portion at the tip. 27a and is fixed by brazing. The first cylindrical part 22b of the intermediate lead body 22 and the cylindrical part 13a of the electrode 13, as well as the cylindrical part 18a of the electrode 13 and the second cylindrical part 22c of the intermediate lead body 22, each work together with the intermediate lead body 22. The first magnetic field generating body 29 and the second magnetic field generating body 30, which constitute the coil 14, are connected in the same direction. 1st
The magnetic field generator 29 and the second magnetic field generator 30 generate an axial magnetic field by changing the current path into a loop centered on the electrode rod 12, as shown in FIGS. 4 and 6. outer ring portions 29a and 30a that fit with the inner peripheral surface of the first cylindrical portion 22b of the intermediate lead body 22 and the inner peripheral surface of the cylindrical portion 18a of the electrode 18 and are fixed by brazing;
The outer peripheral surface of the cylindrical portion 13a of the electrode 13 and the intermediate lead body 2
Inner ring portions 29b and 30b that fit onto the outer peripheral surface of the second cylindrical portion 22C of No. 2 and are fixed by brazing, and the respective outer ring portions 29a and 30a and the inner ring portion 29
1) and 30b through 7! j:'l In order that the flow flows in the same circumferential direction as shown by the arrows, the ring should preferably be formed into an annular shape with an end having an outer diameter intermediate between the two ring parts and provided with radial connecting parts at both ends. It consists of two magnetic field generating parts 29c and 80c, each part of which has a long rectangular cross section extending in the axial direction, and each part is integrally molded.

なお、第4図において31は電極絶縁支持体27の中間
リード体22と電極13とのろう付は時のガス抜き孔で
ある。また、一方(固定側)の電極棒12の内端部に固
着される電極13およびコイル14等は、上述した他方
のものとほぼ同様であるのでその説明を省略する。
In FIG. 4, reference numeral 31 indicates a gas vent hole during brazing between the intermediate lead body 22 of the electrode insulating support 27 and the electrode 13. Further, the electrode 13, coil 14, etc. fixed to the inner end of one (fixed side) electrode rod 12 are substantially the same as the other electrode rod 12 described above, and therefore their explanation will be omitted.

以上の構成からなる真空インタラプタは、従前のものと
同様に幌!作装置によシ対をなす電極13を接離して大
容量の電流を投入、しゃ断するものであり、その通電電
流は、電極棒から中間リード体22の取付部22aに至
るとともに、その第1゜第2円筒部22b、22cK:
おいて分流され、第1、第2円筒部22b 、22cに
至った電流は、第5図に示すように、それぞれ第1磁界
発生体29の外リング部29a、磁界発生部29c、内
リング部29bおよび電極13の円筒部18aを経て電
極13に至るとともに、第2磁界発生体30の内リング
部30b、磁界発生部30c、外リング部30aおよび
電極13の円筒部13aを経て電極13に至る。したが
って、各コイル14は、各磁界発生体29.80の磁界
発生部29c、30cが、径方向へ同心状FC配設され
ることも相俟って、それぞれ外リング部29a、内リン
グ部3obおよび中間リード体22の第1円筒部22b
、第2円筒部22c等を介し電極棒12と接続され、壕
だそれぞれ内リング部29b、外リング部30aおよび
電極13の円筒部13aを介し電極13と接続されるの
で、従来の通電ピンによるものに比して通電断面積が大
きぐなシ発熱等を生ずることがなく、大電流の通電使用
に耐えることができる。
The vacuum interrupter with the above configuration is similar to the previous one. A large amount of current is applied and cut off by connecting and separating the pair of electrodes 13 to the operating device, and the current flows from the electrode rod to the attachment part 22a of the intermediate lead body 22,゜Second cylindrical portion 22b, 22cK:
As shown in FIG. 5, the currents that are divided into the first and second cylindrical parts 22b and 22c are divided into the outer ring part 29a, the magnetic field generator 29c, and the inner ring part of the first magnetic field generator 29, respectively. 29b and the cylindrical portion 18a of the electrode 13 to reach the electrode 13, as well as the inner ring portion 30b of the second magnetic field generator 30, the magnetic field generating portion 30c, the outer ring portion 30a, and the cylindrical portion 13a of the electrode 13 to the electrode 13. . Therefore, in addition to the fact that the magnetic field generating parts 29c and 30c of each magnetic field generating body 29.80 are arranged concentrically in the radial direction, each coil 14 has an outer ring part 29a and an inner ring part 3ob, respectively. and the first cylindrical portion 22b of the intermediate lead body 22
, the electrode rod 12 through the second cylindrical portion 22c, etc., and the groove is connected to the electrode 13 through the inner ring portion 29b, outer ring portion 30a, and cylindrical portion 13a of the electrode 13, so that it can be connected to the electrode 13 through the inner ring portion 29b, the outer ring portion 30a, and the cylindrical portion 13a of the electrode 13. Since the cross-sectional area for current flow is larger than that of other products, it does not generate heat or the like and can withstand use with large currents.

また、各磁界発生体29.30の磁界発生部29c。Moreover, the magnetic field generating part 29c of each magnetic field generating body 29.30.

30c[より発生する軸方向磁界は、全通電電流がそれ
ぞれの磁界発生部29c 、30cに分流されるととも
に、各磁界発生部29c、30cを流れる電流の方向が
同一であるので、通電容−#を高めることができるのは
勿論、第1.第2磁界発生体29.30の磁界発生部2
9 c r 30 cの間隔を出来るだけせまくするこ
とにより、電極13における最初にアークが生ずる平坦
部(接触通電部)18bと対応する第2磁界発生体30
の磁界発生部30cの内側の磁界が強められ、また電極
13の斜面部13Cの周辺と対応する第1磁界発生体2
9の磁界発生部29Cの外側の磁界が強められるととも
に、電極13と鎖交する磁力線の方向が反対となるので
、電Q]8の平坦部13bと斜面部1.3 cとに生ず
る渦電流は逆方向となる。ために、大電流しゃ断直後に
おける渦電流は直ちに相殺されて零となり、軸方向の磁
界と電流の零点とが一致(同位相)となるから、絶縁回
復特性が良好となシ、ひいてはしゃ断絆力を向上するこ
とができる。
The axial magnetic field generated by 30c [with current carrying capacity - Of course, it can improve the first. Magnetic field generating section 2 of second magnetic field generating body 29.30
By making the interval 9c r 30c as narrow as possible, the second magnetic field generator 30 corresponds to the flat part (contact energizing part) 18b where an arc first occurs in the electrode 13.
The magnetic field inside the magnetic field generating section 30c of the first magnetic field generating section 30c is strengthened, and the first magnetic field generating section 2 corresponding to the periphery of the slope section 13C of the electrode 13 is strengthened.
Since the magnetic field outside the magnetic field generating section 29C of 9 is strengthened and the direction of the magnetic lines of force interlinking with the electrode 13 is opposite, eddy currents occur in the flat part 13b and the slope part 1.3c of the electric current Q]8. is in the opposite direction. Therefore, the eddy current immediately after a large current is interrupted is immediately canceled out to zero, and the axial magnetic field and the current zero point coincide (same phase), resulting in good insulation recovery characteristics and, as a result, the breaking bond strength. can be improved.

なお、前述した実施例において1は、中間リード体22
に2個の円筒部22b 、22Cを設けるとともに、電
極13に1個の円筒部18aを設けた場合について述べ
たが、これに限定されるものではなくたとえば逆に電極
13に2個の円筒部を設けるとともに、中間リード体2
2に1個の円筒部を設けてもよいものであり、また、中
間リード体22および電極13のそれぞれに2以上の円
筒部を設けてもよいものである。
Note that in the above-mentioned embodiment, 1 is the intermediate lead body 22.
Although the case has been described in which two cylindrical parts 22b and 22C are provided in the electrode 13 and one cylindrical part 18a is provided in the electrode 13, the present invention is not limited to this. In addition to providing the intermediate lead body 2
2 may be provided with one cylindrical portion, and each of the intermediate lead body 22 and the electrode 13 may be provided with two or more cylindrical portions.

また、前述した実施例においては、同心状の各磁界発生
体29.80の磁界発生部29c、80cを流れる電流
の方向が同一となるように設けた場合について述べたが
、これに限らずたとえば第6図に示すように、それぞれ
の磁界発生部29C230ci、電流が互いに逆方向を
流れるように外リング部29a 、30aおよび内リン
グ29b。
Further, in the above-mentioned embodiment, a case was described in which the magnetic field generating parts 29c and 80c of the concentric magnetic field generating bodies 29.80 were provided so that the direction of the current flowing was the same, but the present invention is not limited to this, for example. As shown in FIG. 6, the respective magnetic field generating portions 29C and 230ci, the outer ring portions 29a and 30a, and the inner ring 29b such that current flows in opposite directions.

30bと接続して設けてもよいものであり、このように
設けることによって、各磁界発生体29゜30により発
生する軸方向磁界が交互に極性の異なる交番MIS界と
なるので、この交番縦磁界により電4夕13に生ずる渦
電流も方向が互いに逆となる。ために、しゃ断時におけ
るしゃ断電流と磁界の位相が一致し、しゃ断性能を向上
することができる。
30b, and by providing it in this way, the axial magnetic fields generated by the magnetic field generators 29 and 30 become alternating MIS fields with different polarities, so this alternating longitudinal magnetic field Therefore, the directions of the eddy currents generated in the electric current 13 are also opposite to each other. Therefore, the phases of the cutoff current and the magnetic field at the time of cutoff match, and the cutoff performance can be improved.

さらに、各磁界発生体29.80の磁界発生部29C,
30cは、有端環状の1個のものとする鳩舎に限らずた
とえば第7図に示すように、それぞれ半円弧状の2個の
ものから形成したシ、または円周方向において3以上に
分割した円弧状のものから形成したり、もしくは外側の
磁界発生部 。
Furthermore, the magnetic field generating portion 29C of each magnetic field generating body 29.80,
30c is not limited to a single ring-shaped pigeon coop with ends, but for example, as shown in Figure 7, a pigeon coop made of two semicircular arc-shaped pieces, or divided into three or more pieces in the circumferential direction. It is formed from an arc-shaped part or an external magnetic field generating part.

’80cを半円弧状の2個または円弧状の3個以上のと
して形成してもよいものであり、このように設けること
により通電容tを一層向上することができるとともに、
磁界発生体29.30からの発熱を均等にすることがで
きる。
'80c may be formed as two semicircular arcs or three or more circular arcs, and by providing them in this way, the current carrying capacity t can be further improved, and
Heat generation from the magnetic field generators 29 and 30 can be made uniform.

また、各磁界発生体29.80の各部は、一体成形する
場合に限らず、別個に形成した各部を接合して形成して
もよいとともに、それぞれの外リング部29a 、30
aおよび内リング部29b。
Further, each part of each magnetic field generating body 29.80 is not limited to being integrally molded, and may be formed by joining each part formed separately, and the respective outer ring parts 29a, 30
a and the inner ring portion 29b.

30bを設けることなく磁界発生部29c、80cのみ
により磁界発生体29.30を形成してもよく、かつ各
磁界発生体29.30を軸方向へ重畳した複数の磁界発
生素体により形成してもよいものである。
The magnetic field generating body 29.30 may be formed only by the magnetic field generating parts 29c and 80c without providing the magnetic field generating body 30b, and each magnetic field generating body 29.30 may be formed by a plurality of magnetic field generating elements superimposed in the axial direction. It's also good.

第8図は本発明の第2実施例の要部縦断面図で、この実
施例のものは、コイル14における第1゜第2磁界発生
体29.30を軸方向へ離隔して設けた2個とするとと
もに、両者間をリング円板状の第1.第2接続導体32
.88により直列接続することによって、軸方向磁界の
強度向上を図ったこと等が前述した第1実施例のものと
相違するものである。ために、第1実施例のものと同一
の部材には同一符号を付してその説明を省略する。
FIG. 8 is a longitudinal cross-sectional view of a main part of a second embodiment of the present invention. In this embodiment, two magnetic field generators 29 and 30 of the coil 14 are provided spaced apart in the axial direction. and a ring-disc-shaped first ring between the two. Second connection conductor 32
.. This embodiment is different from the first embodiment described above in that the strength of the axial magnetic field is improved by connecting the magnets 88 in series. Therefore, the same members as those in the first embodiment are given the same reference numerals and their explanations will be omitted.

すなわち、電極130円筒部13aと中間リード体22
の各円筒部22b 、22cとは、開口端および第2磁
界発生体30がそれぞれ内リング部29bおよび外リン
グ部30aを介し嵌着されており、また中間リード体2
2の第1円筒部22bの内周面および第2円筒部22c
の外周面には、他方の第1磁界発生体29および第2磁
界発生体30がそれぞれ外リング部29aおよび内リン
グ部30bを介して嵌着されている。そして、軸方向へ
離隔されて電極13の円筒部13aの外周面に嵌着した
第1磁界発生体29の外リング部29aと中間リード体
22における第1円筒部22bの内周面に嵌着した第1
磁界発生体29の内リング部29bとは、前記リング円
板状の第1接続導体32における外周縁および内周縁に
互いに異なる軸方向へ突出して形成した突縁82aおよ
び32bを介して電気的に直列接続され、また、同様に
軸方向へ離隔されて電極13の円筒部18a内周面に嵌
着した第2磁界発′生体30の外リング部30aと中間
リード体22における第2円筒部22cの外周面に嵌着
した第2磁界発生体30の内リング部30bとは、前記
リング円板状の第2接続導体33における外周縁および
内周縁に第1接続導体32と同様に形成した突縁33a
および83bを介し電気的に直列接続されている。
That is, the electrode 130 cylindrical portion 13a and the intermediate lead body 22
The open end and the second magnetic field generator 30 are fitted into the cylindrical parts 22b and 22c through the inner ring part 29b and the outer ring part 30a, respectively, and the intermediate lead body 2
2, the inner circumferential surface of the first cylindrical portion 22b and the second cylindrical portion 22c
The other first magnetic field generating body 29 and second magnetic field generating body 30 are fitted onto the outer peripheral surface of the magnetic field generating body 29 through an outer ring portion 29a and an inner ring portion 30b, respectively. Then, the outer ring part 29a of the first magnetic field generator 29, which is spaced apart in the axial direction and fitted onto the outer peripheral surface of the cylindrical part 13a of the electrode 13, is fitted into the inner peripheral surface of the first cylindrical part 22b of the intermediate lead body 22. The first
The inner ring portion 29b of the magnetic field generator 29 is electrically connected to the inner ring portion 29b of the ring disk-shaped first connection conductor 32 through projecting edges 82a and 32b formed on the outer and inner edges of the ring disk-shaped first connection conductor 32 so as to protrude in mutually different axial directions. The outer ring portion 30a of the second magnetic field generator 30 and the second cylindrical portion 22c of the intermediate lead body 22 are connected in series and are similarly spaced apart in the axial direction and fitted onto the inner peripheral surface of the cylindrical portion 18a of the electrode 13. The inner ring part 30b of the second magnetic field generating body 30 fitted on the outer peripheral surface of the second magnetic field generating body 30 is a protrusion formed on the outer peripheral edge and the inner peripheral edge of the second connecting conductor 33 in the shape of a ring disk in the same manner as the first connecting conductor 32. Rim 33a
and 83b are electrically connected in series.

なお、上述した第2実施例においては、中間リード体2
2の円筒部22b、22cを2個とし、電極13の円筒
部13aを1個とした場合について例示しであるが、こ
れに限定されるものではなく、第1実施例の場合と同様
に電極13の円筒部13 a f 2個とし、中間リー
ド体22の円筒部を1個としてよいのは勿論、電極18
の円筒部および中間リード体22の円筒部をそれぞれ2
個以上としてもよいものである。
Note that in the second embodiment described above, the intermediate lead body 2
The cylindrical portions 22b and 22c of the second embodiment are two, and the cylindrical portion 13a of the electrode 13 is one. However, the present invention is not limited to this. Of course, the cylindrical portions 13 a f of 13 may be two, and the cylindrical portion of the intermediate lead body 22 may be one.
and the cylindrical portion of the intermediate lead body 22, respectively.
It is also possible to have more than one.

また、各磁界発生体29.30は、前述した第1実姉例
の場合と同様にその態様を種々変更し得るのは勿論であ
り、かつ外リング部29a、30aおよび内リング部2
9b 、80bは、少なくともいずれか一方を備えてお
ればよいものである。
In addition, it goes without saying that each magnetic field generator 29, 30 can be modified in various ways as in the case of the first sister example described above, and the outer ring portions 29a, 30a and the inner ring portion 29.
It is sufficient that at least one of 9b and 80b is provided.

以上の如く本発明は、真空容器内に1 ?jの電極棒を
軸線上に位置せしめて相対的に接近離反自在に導入し、
前記各電極棒の内端部に、1または同心状の2以上の円
筒部を備えた中間リード体をその円筒部の開口端を対向
せしめて同心的に固着するとともに、中間リード体の円
筒部と径を違えた1または同心状の2以上の円筒部を背
部に備えた電極をその円筒部を中間リード体の円筒部と
半径方向において同心状に交互に重畳せしめ電極絶縁支
持体を介して直列的に固着し、前記各中間り一ド体の円
筒部と相隣るそれぞれの電極の円筒部とを有端環状また
は円周方向において2以上に分割した円弧状の磁界発生
体により接続して設けたものであるから、従来のものの
ようにコイルと電極との接続部における抵抗熱の発生等
によシ通電容量が規制されることはないとともに、大容
量の電流を優れたしゃ断性能でしゃ断することができ、
かつ軸方向磁界の強度および分布を容易に設定できる等
の効果を奏する。
As described above, in the present invention, 1 ? The electrode rod j is positioned on the axis and introduced so that it can be relatively approached and separated,
An intermediate lead body having one or two or more concentric cylindrical parts is concentrically fixed to the inner end of each of the electrode rods with the open ends of the cylindrical parts facing each other, and the cylindrical part of the intermediate lead body An electrode having one or two or more concentric cylindrical parts with different diameters on the back side, the cylindrical parts are alternately overlapped concentrically in the radial direction with the cylindrical part of the intermediate lead body, and the electrodes are interposed through an electrode insulating support. fixed in series, and connecting the cylindrical portion of each intermediate one-piece body and the cylindrical portion of each adjacent electrode by a magnetic field generating body having an end ring shape or an arc shape divided into two or more in the circumferential direction. Since the current carrying capacity is not restricted due to the generation of resistance heat at the connection between the coil and the electrode, unlike conventional ones, it is also possible to handle large currents with excellent breaking performance. can be cut off,
Moreover, it is possible to easily set the strength and distribution of the axial magnetic field.

また、真空容器内に1対の電極棒を軸線上に位置せしめ
て相対的に接近離反自在に導入し、前記各電極棒の内端
部に、1または同心状の2以上の円筒部を備えた中間リ
ード体をその円筒部の開口端を対向せしめて同心的に固
着するとともに、中間リード体の円筒部と径を違えた1
ま念は同心状の2以上の円筒部を背部に備えた電極をそ
の円筒部の開口端と中間リード体の円筒部の開口端とを
軸方向へ離隔しかつその円筒部を中間リード体の円筒部
と半径方向において同心状に交互に重畳せしめるが如く
し電極絶縁支持体を介して直列的に固着し、前記各中間
リード体の円筒部および相隣るそれぞれの電極の円筒部
に外リング部および内リング部の双方またはいずれか一
方を備えた有端環状または円周方向において2以上に分
割した円弧状の磁界発生体を嵌着し、前記各中間リード
体の円筒部に嵌着した磁界発生体とそれぞれの電極の円
筒部に嵌着した磁界発生体とをリング円板にしてかつ内
周縁および外周縁に突縁を備えた接続導体により直列接
続したものであるから、上述した効果に加えて軸方向磁
界の強度を大幅に向上することかできる等の効果を奏す
る。
Further, a pair of electrode rods are positioned on the axis line and introduced into the vacuum container so as to be able to approach and separate from each other, and each electrode rod has one or two or more concentric cylindrical portions at the inner end thereof. The intermediate lead body is fixed concentrically with the open end of the cylindrical part facing each other, and the diameter is different from that of the cylindrical part of the intermediate lead body.
The idea is to use an electrode with two or more concentric cylindrical parts on the back, and to separate the open end of the cylindrical part from the open end of the cylindrical part of the intermediate lead body in the axial direction, and to separate the cylindrical part from the open end of the cylindrical part of the intermediate lead body. An outer ring is attached to the cylindrical portion of each intermediate lead body and the cylindrical portion of each adjacent electrode, and is fixed in series through an electrode insulating support such that the cylindrical portion and the cylindrical portion are alternately overlapped concentrically in the radial direction. A magnetic field generating body having an end ring shape or an arc shape divided into two or more parts in the circumferential direction is fitted into the cylindrical part of each of the intermediate lead bodies. Since the magnetic field generator and the magnetic field generator fitted into the cylindrical portion of each electrode are formed into ring disks and are connected in series by a connecting conductor having protrusions on the inner and outer edges, the above-mentioned effects can be achieved. In addition to this, the strength of the axial magnetic field can be significantly improved.

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

第1図および第2図はそれぞれ従来の真空インタラプタ
の要部の縦断面図および平面図、第3図は本発明に係る
真空インタラプタの縦断面図、第4図は本発明の第1実
施例の要部縦断面図、第5図は第4図におけるV−V線
断面図、第6図および第7図はそれぞれ第1実施例にお
ける要部の他の実施例の横断面図、第8図は本発明の第
2実施例の要部の縦断面図である。 11・・・真空容器、12・・・電極棒、13・・・電
極、18a・・・円筒部、22・・・中間リード体、2
2b。 22C・・・円筒部、27・・・電、極絶縁支持体、2
9゜30・・・磁界発生体、32.33・・・接続導体
、32a。 82 b 、 83 a 、 33 b ・−突縁。 1 第1図 第2図
1 and 2 are a vertical cross-sectional view and a plan view of the main parts of a conventional vacuum interrupter, respectively, FIG. 3 is a vertical cross-sectional view of a vacuum interrupter according to the present invention, and FIG. 4 is a first embodiment of the present invention. FIG. 5 is a cross-sectional view taken along the line V-V in FIG. 4, FIGS. 6 and 7 are cross-sectional views of other embodiments of the main part of the first embodiment, and FIG. The figure is a longitudinal sectional view of the main part of the second embodiment of the present invention. DESCRIPTION OF SYMBOLS 11... Vacuum container, 12... Electrode rod, 13... Electrode, 18a... Cylindrical part, 22... Intermediate lead body, 2
2b. 22C...Cylindrical part, 27...Electrode, electrode insulating support, 2
9°30...Magnetic field generator, 32.33...Connecting conductor, 32a. 82 b, 83 a, 33 b - ridge. 1 Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 (1)真空容器内に1対の電極棒を軸線上に位置せしめ
て相対的に接近離反自在に導入し、前記各電極棒の内端
部に、1または同心状の2以上の円筒部を備えた中間リ
ード体をその円筒部の開口端を対向せしめて同心的に固
着するとともに、中間リード体の円筒部と径を違えた1
または同心状の2以上の円筒部を背部に備えた電極をそ
の円筒部を中間リード体の円筒部と半径方向において同
心状に交互に重畳せしめ電極絶縁支持体を介して直列的
に固着し、前記各中間リード体の円筒部と相隣るそれぞ
れの電極の円筒部とを有端環状または円周方向において
2以上に分割した円弧状の磁界発生体により接続して設
けたことを特徴とする真空インタラプタ。 (2)  同心状の磁界発生体を11イ流が同一方向へ
流れるようにして中間リード体の円筒部および電極の円
筒部と接続したことを特徴とする特許請求の範囲第1項
記載の真空インタラプタ。 (3) 同心状の磁界発生体を電流が交互に方向を変え
て流れるようにして中間リード体の円筒部および電極の
円筒部と接続したことを特徴とする特許請求の範囲第1
項記載の真空インタラプタ。 (4)  同心状の磁界発生体の内側のものを有端環状
のものとするとともに外側のものを2以上の円弧状のも
のとしたことを特徴とする特許請求の範囲第1項から第
3項までのいずれかに記載の頁、空インタラプタ。 (5)磁界発生体を軸方向へ重畳した2以上の磁界発生
素体によ多形成したことを特徴とする特許請求の範囲第
1項から第4項1でのいずれかに記載の真空インタラプ
タ。 (6)磁界発生体を中間リード体の円筒部または電極の
円筒部に嵌着される外リング部および内リング部を備え
たものとしたことを特徴とする特許請求の範囲第1項か
ら第5項までのいずれかに記載の真空インタラプタ。 (7)真空容器内に1対の電極棒を軸線上に位置せしめ
て相対的に接近離反自在に導入し、前記各電極棒の内端
部に、1または同心状の2以上の円筒部を備えた中間リ
ード体をその円筒部の開口端を対向せしめて同心的に固
着するとともに、中間リード体の円筒部と径を違えた1
捷たは同心状の2以上の円筒部を背部に備えた電極をそ
の円筒部の開口端と中間リード体の円筒部の開口端とを
軸方向へ離隔しかつその円筒部を中間リード体の円筒と
半径方向において同心状に交互に重畳せしめるが如くし
電極絶縁支持体を介して直列的に固着し、前記各中間リ
ード体の円筒部および相隣るそれぞれの電和メの円筒部
に外リング部および内リング部の双方捷たはいずれか一
方を備えた有端環状普たけ円周方向において2以上に分
割した円弧状の磁界発生体を嵌着し、前記各中間リード
体の円筒部に嵌着した磁界発生体とそれぞれの電極の円
筒部に嵌着した磁界発生体とをリング円板状にしてかつ
内周縁および外周縁に突縁を備えた接続導体により直列
1厘続して設けたことを特徴とする真空インタラプタ。 (8)  同心状の磁界発生体を電流が同一方向へ流れ
るようにして中間リード体の円筒部および電極の円筒部
と接続したこと全特徴とする特許請求の範囲第7項記載
の真空インタ2プタ。 (9)  同心状の磁界発生体を電流が交互に方向を変
えて流れるようにして中間リード体の円筒部および電極
の円筒部と接続したことを特徴とする特許n請求の範囲
第7項記載の真空インタラプタ。 (11同心状の磁界発生体の内側のものを有端環状のも
のとするとともに外側のものを2以上の円弧状のものと
したことを特徴とする特許請求の範囲第7項から第9項
までのいずれかに記載の真空インタラプタ。 (11)磁界発生体を軸方向へ重畳した2以上の磁界発
生素体により形成したことを特徴とする特許請求の範囲
第7項から第10項までのいずれかに記載の真空インタ
2ブタ。
[Scope of Claims] (1) A pair of electrode rods are positioned on the axis line and introduced into a vacuum container so as to be able to approach and separate from each other, and one or a concentric electrode is inserted into the inner end of each of the electrode rods. An intermediate lead body having two or more cylindrical parts is fixed concentrically with the open ends of the cylindrical parts facing each other, and the diameter is different from that of the cylindrical part of the intermediate lead body.
Alternatively, an electrode is provided with two or more concentric cylindrical parts on the back, and the cylindrical parts are alternately overlapped concentrically in the radial direction with the cylindrical part of the intermediate lead body, and the electrodes are fixed in series via an electrode insulating support, The cylindrical portion of each intermediate lead body and the cylindrical portion of each adjacent electrode are connected by a magnetic field generating body having an end ring shape or an arc shape divided into two or more parts in the circumferential direction. Vacuum interrupter. (2) A vacuum according to claim 1, characterized in that a concentric magnetic field generating body is connected to the cylindrical part of the intermediate lead body and the cylindrical part of the electrode so that the 11 currents flow in the same direction. Interrupter. (3) The first aspect of the present invention is characterized in that the concentric magnetic field generators are connected to the cylindrical portion of the intermediate lead body and the cylindrical portion of the electrode in such a manner that current flows through the concentric magnetic field generators while changing directions alternately.
Vacuum interrupter as described in section. (4) Claims 1 to 3, characterized in that the inner part of the concentric magnetic field generator is annular with ends, and the outer part is in the shape of two or more circular arcs. Pages listed in any of the sections up to the empty interrupter. (5) The vacuum interrupter according to any one of claims 1 to 4, 1, characterized in that the magnetic field generating body is formed of two or more magnetic field generating elements superimposed in the axial direction. . (6) Claims 1 to 1, characterized in that the magnetic field generator is provided with an outer ring portion and an inner ring portion that are fitted into the cylindrical portion of the intermediate lead body or the cylindrical portion of the electrode. The vacuum interrupter according to any one of items 5 to 5. (7) A pair of electrode rods are positioned on the axis line and introduced into the vacuum container so that they can be moved toward and away from each other, and one or more concentric cylindrical portions are attached to the inner end of each electrode rod. The intermediate lead body provided with the intermediate lead body is fixed concentrically with the open end of the cylindrical part facing each other, and the diameter is different from that of the cylindrical part of the intermediate lead body.
An electrode having two or more twisted or concentric cylindrical parts on its back is separated in the axial direction from the open end of the cylindrical part and the open end of the cylindrical part of the intermediate lead body, and the cylindrical part is separated from the open end of the cylindrical part of the intermediate lead body. The electrodes are alternately overlapped concentrically with the cylinder in the radial direction, and are fixed in series through the electrode insulating support, and are externally attached to the cylindrical part of each of the intermediate lead bodies and the cylindrical part of each adjacent electrical wire. An arcuate magnetic field generating body divided into two or more in the circumferential direction is fitted into the circular arc-shaped magnetic field generator having both or one of the ring part and the inner ring part, and the cylindrical part of each intermediate lead body. The magnetic field generating body fitted into the cylindrical part of each electrode and the magnetic field generating body fitted into the cylindrical part of each electrode are formed into a ring disc shape and are connected in series by a connecting conductor having protruding edges on the inner and outer peripheral edges. A vacuum interrupter characterized by the following: (8) The vacuum interconnect 2 according to claim 7, characterized in that concentric magnetic field generators are connected to the cylindrical portion of the intermediate lead body and the cylindrical portion of the electrode so that current flows in the same direction. Puta. (9) Claim 7 of the patent, characterized in that the concentric magnetic field generators are connected to the cylindrical portion of the intermediate lead body and the cylindrical portion of the electrode in such a manner that current flows through the concentric magnetic field generators while changing directions alternately. vacuum interrupter. (Claims 7 to 9) characterized in that the inner part of the concentric magnetic field generator is annular with ends, and the outer part is in the shape of two or more circular arcs. (11) The vacuum interrupter according to any one of claims 7 to 10, characterized in that the magnetic field generating body is formed by two or more magnetic field generating elements superimposed in the axial direction. The vacuum inter-tube according to any one of the above.
JP1267582A 1982-01-29 1982-01-29 Vacuum interrupter Pending JPS58129718A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1267582A JPS58129718A (en) 1982-01-29 1982-01-29 Vacuum interrupter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1267582A JPS58129718A (en) 1982-01-29 1982-01-29 Vacuum interrupter

Publications (1)

Publication Number Publication Date
JPS58129718A true JPS58129718A (en) 1983-08-02

Family

ID=11811943

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1267582A Pending JPS58129718A (en) 1982-01-29 1982-01-29 Vacuum interrupter

Country Status (1)

Country Link
JP (1) JPS58129718A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01159418U (en) * 1988-04-22 1989-11-06
JP2009252388A (en) * 2008-04-02 2009-10-29 Japan Ae Power Systems Corp Large-capacity vacuum circuit breaker

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01159418U (en) * 1988-04-22 1989-11-06
JP2009252388A (en) * 2008-04-02 2009-10-29 Japan Ae Power Systems Corp Large-capacity vacuum circuit breaker

Similar Documents

Publication Publication Date Title
EP0113962A1 (en) Vacuum interrupter
JPS58129718A (en) Vacuum interrupter
JPS6336916Y2 (en)
JPS6336918Y2 (en)
JPS6347218B2 (en)
JPH0427650B2 (en)
JPS6318292B2 (en)
JPS5847628Y2 (en) Vacuum cutter
JPS5849975B2 (en) Vacuum cutter
JPS6347219B2 (en)
JPS6328829Y2 (en)
JPS6245401Y2 (en)
JPS645325Y2 (en)
JPS6313634Y2 (en)
JPS6313635Y2 (en)
JPS5951427A (en) Vacuum interrupter
JPS63236228A (en) Vacuum interruptor
JPS5923422A (en) Vacuum interrupter
JPS6214581Y2 (en)
JPS5848321A (en) Vacuum breaker
JPS6166324A (en) Vacuum interrupter
JPS5848322A (en) Vacuum breaker
JPS6231917A (en) Electrode construction of vacuum discharge-applied equipment
JPH0123891B2 (en)
JPS6319969B2 (en)