JPS5951427A - Vacuum interrupter - Google Patents

Vacuum interrupter

Info

Publication number
JPS5951427A
JPS5951427A JP16183382A JP16183382A JPS5951427A JP S5951427 A JPS5951427 A JP S5951427A JP 16183382 A JP16183382 A JP 16183382A JP 16183382 A JP16183382 A JP 16183382A JP S5951427 A JPS5951427 A JP S5951427A
Authority
JP
Japan
Prior art keywords
coil
electrode
magnetic field
vacuum interrupter
outer diameter
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.)
Granted
Application number
JP16183382A
Other languages
Japanese (ja)
Other versions
JPS6319054B2 (en
Inventor
佐野 孝光
川上 秀雄
芦沢 喬
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 JP16183382A priority Critical patent/JPS5951427A/en
Publication of JPS5951427A publication Critical patent/JPS5951427A/en
Publication of JPS6319054B2 publication Critical patent/JPS6319054B2/ja
Granted 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】[Detailed description of the invention]

本発明は真空インタラプタに係り、特にアークに対して
平行な軸方向磁界ケ発生させる手段を電極の周辺に備え
てなる真空インタラプタに関する。 従来、軸方向の磁界(縦磁界)V発生させる手段を電極
の周辺に備えてなる真空インタラプタは。 通常、ガラス等から絶縁筒の両開ロ部ケ両端に固着した
封着金具ケ介し金属端板忙より閉塞しかつ内部を高真空
に排気して真空容器V形成し、この真空容器内に円板状
ケな−t1対の電極ケ各金属端板の中央から相対的に接
近離反自在に導入した対!なす電極棒!介し機械的に接
触離反(接離)自在に設けるとともに、各電極とそ几ぞ
nの電極棒とを同一極性の軸方向磁界を発生すべくそ几
ぞれの電極の背部
The present invention relates to a vacuum interrupter, and more particularly to a vacuum interrupter comprising means around an electrode for generating an axial magnetic field parallel to an arc. Conventionally, a vacuum interrupter is provided with means for generating an axial magnetic field (vertical magnetic field) V around an electrode. Usually, the double-opening opening part of the insulating cylinder is closed off from the metal end plate through sealing fittings fixed to both ends of the insulating cylinder, and the inside is evacuated to a high vacuum to form a vacuum vessel V, and a circle is placed inside the vacuum vessel. A pair of plate-shaped electrodes introduced from the center of each metal end plate so that they can approach and separate from each other! Eggplant electrode rod! In addition to mechanically providing mechanical contact and separation (contact and separation), each electrode and its respective electrode rods are connected to the back of each electrode in order to generate an axial magnetic field of the same polarity.

【配置した有端環状または周方向へ2
月上に分割さnた環状にしてかつ電、極とほぼ同外径の
コイル?介し電気的に直列接続して構成さnている。 しかしながら、従来の軸方向磁界方式の真空インタラプ
タは、電極の従離により生ずるアーク?軸方向磁界によ
り電極間空間に閉じ込めてその安定化を図り、もってし
ゃ新客tv径方向(横)磁界方式のものより増大するこ
とができるものの。 その電極面におけるアークスポットが、電極の外周部付
近には点在しないとともにその中央付近またはその中心
?中心とする同心円上に集中して偏在し、′電極面を有
効に活用し得ない問題がある。 かかる中線は、同一極性σ〕磁界を発生寸ろ2個のコイ
ルヶ軸方向へ所定間隔離隔するとともに。 両者同一にしてその外径’&f化させて、両コイルによ
る合成された軸方回磁界の径方向の分布状態ケ副定した
実験結果ケ示す駆1図か島も明らかな如く、合成さ几た
軸方回磁界σ)径方向の外布状態が不均一であることに
依ると思わ几る。−tなわち。 第1図は横軸にコイルσ)外径R′lX′、縦軸に合成
さnた軸方回磁界の強lfH%−とり、コイルσ)外径
R?変化させた場合の合放さ几た軸方回磁界の径方向の
分布状態?、コイルの外径Rσ】増大θ)順r曲(lA
、B、CおよびDで示したもので、こ7″L、Vr、よ
ればコイルσ〕外径Rが小さい噛合には1曲線Aで示す
よ′1に1合成軸方回磁界の強度Hがコイルの中心0に
おいて最高となる凸状ケ呈し、またコイルの外径Rが大
きい場合には、曲iWB 、 CおよびDで示寸よ5K
、合成軸方回磁界の強度Hがコイルの中心0匠おいて最
低となりかつコイルの内周部付近において最高となる凹
状ケ呈するとともに、コイルの外径Rの増大につれて最
低点および最高点が低下する傾向にあり、合成軸方回磁
界、すなわち磁束密度の径方向の分布が不均一となるこ
とにより、アークスポットの偏在を招来していることが
判るものである。 本発明は上述した間@r艦みてなさnたもので。 その目的とするところは、対をな−t″電極棒を介し一
α空容器内において機械的に接離自在に設け′ら几る1
対の電極の外周に凹状の軸方向磁界を発生すべく1また
は2以上の軸方向のスリブ)V有する円筒状の筆1コイ
ルケ同心配@するとともに、いず几か一方または他方の
電極の背部に凸状にしてかつ$1コイルより強度σ)小
さい軸方向磁界?発生すべく箪1コイルより小径にして
かつ周方向の分割数を多くした環状の第2コイルケ同心
配置し、こT′L、l−1の箪1コイルおよび第2コイ
ルを同一極性の磁界′%−発生すべくそれぞれいす几か
一方または他方の電極棒と電極とに゛ε電気的接続する
ことにより1両コイルによる合成軸方向磁界の径方向の
分布状態ケミ極面全面に亘って均一にしてアークスポッ
トの均一な拡散を図り、もって電極面ケ有効に活用し得
るよろにした軸方向磁界方式の真空インタラプタV操供
するにある。以下、駆2図以降の図面′?参照してこの
発明の実施例を詳細に説明する。 第2図は本発明に係る真空インタラプタの縦断面図で、
この真空インタラプタは、円筒状に形成シタガラス、セ
ラミックス等かへなる2本の絶縁筒1,1.yI/、両
端に固着したコバール等からなろ薄丙円環状の封着金具
2・2・°°°の一方?介し同軸的に接合
[Arranged in an annular shape with ends or in the circumferential direction 2
Is it a coil that is divided into a ring shape on the moon and has an outer diameter that is almost the same as the electrode and pole? They are electrically connected in series through the two. However, conventional axial magnetic field type vacuum interrupters suffer from arcing caused by separation of electrodes. The axial magnetic field is used to confine the magnetic field in the interelectrode space and stabilize it, which can be increased compared to the radial (horizontal) magnetic field method. Are the arc spots on the electrode surface not scattered near the outer periphery of the electrode, and near or at the center? There is a problem in that the electrode surface is concentrated and unevenly distributed on the concentric circle at the center, making it impossible to effectively utilize the electrode surface. Such a median line generates a magnetic field of the same polarity σ] and is spaced apart by a predetermined distance in the axial direction of the two coils. The results of the experiment in which the radial distribution state of the combined axial rotating magnetic field by both coils was determined by making both the same and making their outer diameters '&f' are the same, as is clear from Figure 1. This is thought to be due to the non-uniformity of the outer distribution in the radial direction. -t that is. In Figure 1, the horizontal axis represents the coil σ) outer diameter R′lX′, the vertical axis represents the strength lfH% of the combined axial magnetic field, and the coil σ) outer diameter R? What is the radial distribution state of the combined axially rotating magnetic field when the magnetic field is changed? , coil outer diameter Rσ】increase θ) order r curve (lA
, B, C, and D, and for meshing with a small outer diameter R, the intensity of the combined axial magnetic field H is shown by curve A. If the coil has a convex shape that is highest at the center 0 of the coil, and the outer diameter R of the coil is large, the curves iWB, C, and D should be 5K.
, the strength H of the composite axial magnetic field is lowest at the center of the coil and highest near the inner circumference of the coil, exhibiting a concave shape, and as the outer diameter R of the coil increases, the lowest and highest points decrease. It can be seen that the composite axial magnetic field, that is, the distribution of the magnetic flux density in the radial direction becomes non-uniform, leading to uneven distribution of arc spots. The present invention was developed based on the above-mentioned features. The purpose of this is to provide a pair of electrodes that can be mechanically brought into contact with and separated from each other in an empty container via a pair of electrode rods.
To generate a concave axial magnetic field on the outer periphery of the pair of electrodes, a cylindrical brush with one or more axial slits (concentric) and one or more axial ribs (concentric) and one or more of the backs of one or the other electrode. A convex shape and a smaller axial magnetic field than the $1 coil? In order to generate a magnetic field of the same polarity, a second annular coil with a diameter smaller than that of the first coil and a larger number of divisions in the circumferential direction is arranged concentrically. % - By electrically connecting one or the other electrode to the electrode, the radial distribution of the combined axial magnetic field from one coil can be made uniform over the entire surface of the chemical pole. A vacuum interrupter V of the axial magnetic field type is used, which aims to uniformly diffuse the arc spot and thereby make effective use of the electrode surface. Below are the drawings from Kaku 2 onwards. Embodiments of the present invention will be described in detail with reference to the drawings. FIG. 2 is a longitudinal cross-sectional view of the vacuum interrupter according to the present invention.
This vacuum interrupter consists of two cylindrical insulating cylinders 1, 1. yI/, one of the thin circular ring-shaped sealing fittings 2, 2, °°° made of Kovar etc. fixed on both ends? Coaxially joined through

【−て1本の
絶縁筒とするとともに。 その両開口部?他方の封着金具2.2ケ介しステンレス
鋼等がちなる円板状の金属端板3.3により閉塞し、か
つ内部を高真空に排気して真空容器4ヶ形成し、この真
空容器4内にほぼ同外径の円板状7なす1対の雷、極5
.6を各金属端板3,3の中央部から真空容器4の気密
性?保持して相対的に接近離反自在に導入した対をなす
電極棒7゜8ケ介し後述する如く機械的に接離自在に設
け、1対の電極5.6の外周に軸方向(第2図において
上下方向)のスリットを有する円筒状の軍1コイル9を
同心配置1するとともに、第1コイル9と相俟って電極
5.6間における径方向(箪2図において左右方向)の
磁界分布ケ均一に寸べく、固定側(第21ゾにおいて上
側)0)電極5の背部にこの′1極5と同径にしてかつ
円周方間の分割数?第1コイル9より多くした環状の第
2コイル10X(+/固定側電極棒7Vr対して同心配
置し、駆1コイル9および第2コイル10i同一極性の
軸方向磁界ケ発生すべくそnぞ几固定側電極棒7と固定
側電極5とに電気的に接続して概略構成さnている。 すなわち、固定111IIl電極棒7の内端部には、第
3図に示すよ5に、はぼ半円形の突出部7aと段部7b
が形成さ几ており1段部7bKは、セラミックスのη口
きS練物またはステンレス鋼、ハステロイ、インコネル
等の如き高抵抗の金属からなり、突出部7aの高さと同
等の厚さ?有する円板状のスペーサ11の一面が固着さ
れている。そして、固定側電極棒7の突出部7aの端面
とスペーサ11の他面には、第3図および第4図に示す
よ5に。 電極棒7の外径より適宜大きい外径?有する円筒形にし
てかつ軸方向のスリット12%’有するコイル部9aと
、コイル部9aの一方の筒端(第3図において上端)か
らスリツ)12V間にして半径方向(箪2図において左
右方向)内方へ平行に延伸した箪】接続腕9bおよび第
2接続腕9cとからなる前記$1コイル9が、第1接続
腕9bと第2接続腕9cの端部に形成した半円形の接続
部を介しそのコイル部9aケ固定1111I市、極棒7
に対し直列配置となるが如くして取付けちれている。 前記筆1コイル9における軍2接続腕9cの端部には、
一端面にほぼ半円形の突出部13dと段部13fi%’
形成した補助電極棒13が、固定側電極棒71f対し直
列配置となるが如くし突出部13fiの端面ケ介して固
着されているとともに、第1接続腕9hの端部には、絶
縁物または高抵抗の金属からなり、−面ケ補助電極棒1
3の段部13hK組 固着した円板状のスペーサ14の他端が固着さ几ている
。補助電極棒13の他端面には1円形の凹部15が設け
1l−1rt、ており、この凹部15には、絶縁物また
は高抵抗の金属からなりかつ凹部15の深さと同程度の
長さケ有する円筒状のスペーサ16か、一端ケ凹部15
の底部に固着して同心状に収納さnている。スペーサ1
6の他端および゛補助電極棒13の他端面には、駆3図
、第5図に示すように、凹部15の内径より適宜小径の
円柱状に形 0 成した電極接続部to、1と、市、極接続10aO)外
周面における4等分した位置から半径方向外方へ延伸し
た4本の第1腕部iob、1ob、・・・と。 各@1@部10bの端部かf−1箪1コイル9の約40
〜70%(本実施例においては約60%)の曲率半径で
ほぼ174周ずつ同−円周方向へ彎曲した4個のコイル
部10c、10c、・・・と、各コイル部10cの端部
からそ几ぞれの第1腕部10bと平行に半径方向内方へ
延伸した4本の第2腕部10d。 10d、・・・と、各第2腕部10dの端部から凹部1
5の内径および補助電極棒13の外径ケ内、外反対の同
−円周方向へ彎曲した4個の電極棒接続部10e110
e、…とからなる前記第2コイル】0が、電極接続部1
0fiおよび各電極棒接続部1 108の一婦ケ介して固着さ几ている。そして、第2コ
イル10における電極接続部IQq171他端には、駆
2コイル10とほぼ同径の円板状に形成された前記固定
1IIl+の電極5が、その背面(第3図において上面
)中央に設けた凹部17?介し第1コイル9の各磁界発
生部1(lcから離隔さnろが如くして嵌着さ几ており
、また、可か側の電極棒8σ)内端には、固定側の電極
5と同径の円板状に形成さnた前記可動側の電極6が、
その背面(第、iへ 3図において下面)中央に設けた凹部な介して嵌着され
ている。 なお、第2図において19は金属ベローズ、20は各電
極5.6および第1コイル9等ケ同心状に囲繞する中間
シールド、21.21は各金属端板3の内面に固着した
補助シールドである。また、】 2 筆3図において22は筆2コイル10′?補強支持すべ
く補助電極棒13Vr嵌着したリング円板状のコイル補
強部材で、高抵抗の金属等からなるものであるとともに
、W、xコイル9も図示しない同様のコイル補強部材ケ
介して補強支持さ几ているものであり、23は補助電極
棒13の他端に設けた切欠で、第2コイル10の第1腕
部10bと補助電極棒13とが電気的に直接導通ずるの
?防止するためのものである。 以上の構成の箪1実施例の真空インタラプタによる主回
路′llr流のしゃ断は、通常の真空インタラプタと同
様に、電極5.6の開離によって両者間に生じたアーク
か、電極5.6が十分に開離されるとともに電流が自然
零値またはその近傍に至って消滅することにより完了す
るものであるが、甫3 極5.6間に発生したアークは、横軸にコイル外径R1
縦軸に軸方向磁界Hvとるとともに、両コイル9 、1
0により生ずる軸方向磁界ケ曲1gAA、    ′B
で示し、また両軸方向磁界を合成した軸方向磁界ケ曲m
cで表わした第6図に示すよ’SK、’811コイル9
と第2コイル10とにより径方向に亘ってほぼ均一な強
さの軸方向磁界が印加さ几ることになるので、そのアー
クスポットが両電極5.Rの対間する面全面に亘りほぼ
均一に拡散されるものである。 なお、上述した実施例においては、@2コイル10%’
固定側電極5の背部に配置した場合について述べたが、
こnに限定さnるものではなく、たとえば可動側電極6
の背部に配置してもよいものであるとともIC,lE1
コイル9も同様に、可動側 4 の電極棒8等と電気的KW続してもよいものである。ま
た、筆1コイル9は軸方向のスリット12ヶ1個設けた
いわゆる1ターンタイプのものに限らず、筆2コイル1
0の分割数より少ない範囲内において分割数?多くして
もよいものである。さ11−1に、真空容器4は、2本
の絶縁筒1かへなる1本の絶縁筒とその両端を閉塞する
金属端板3.3とから形成する場合に限らず、たとえば
1本または3本以上の絶縁筒とその両端ゲ閉塞する2枚
の金属端板とから形成したり、金属筒とその両端ケ閉塞
する絶縁端板とから形成してもよいのは勿論である。 以上の如く本発明は、真空容器内に1対の電極?相対的
に接近離反自在に導入した対をな−f′電極棒を介し機
械的に接離自在に設け、前記対?なす5 電、極の外周Vr1または2N上の軸方向スリットを有
する円筒状の第1コイルケ同心配置するとともに、前記
いずnか一方または他方の電極の背部に箪1コイルより
小径にしてかつ周方向の分割数ケ多くした環状の第2コ
イルを配置し、前記第1コイルおよび第2コイルケ同一
極性び】磁界ケ発生すべくそれぞれいず几か一方または
他方の電極棒と電極とに電気的VC接続したものである
から、しゃ断時に電極間に発生するアークのスポット’
v 電qt面全面に狂り均一に拡散することができ、ひ
いてはしゃ新客tv効率よく増大することができる等の
効果ケ奏する。
[- and make it into one insulating tube. Both openings? The other sealing fitting 2.2 is closed with a disc-shaped metal end plate 3.3 made of stainless steel or the like, and the inside is evacuated to a high vacuum to form four vacuum vessels. A pair of disk-shaped lightnings 7 with approximately the same outer diameter, poles 5
.. 6 from the center of each metal end plate 3, 3 to the airtightness of the vacuum container 4? A pair of electrode rods 7.8 are held and introduced so as to be able to approach and separate from each other mechanically, as will be described later. A cylindrical first coil 9 having a slit in the vertical direction (in the vertical direction) is arranged concentrically 1, and together with the first coil 9, the magnetic field distribution in the radial direction (in the horizontal direction in Fig. 2) is created between the electrodes 5.6. To ensure uniform size, the back of the fixed side (upper side in the 21st part) electrode 5 has the same diameter as the electrode 5 and the number of divisions in the circumferential direction. An annular second coil 10X (more than the first coil 9) (+/ arranged concentrically with respect to the fixed electrode rod 7Vr, and fixed in place in order to generate an axial magnetic field of the same polarity as the first coil 9 and the second coil 10i) It is electrically connected to the side electrode rod 7 and the stationary side electrode 5. That is, at the inner end of the stationary electrode rod 7, as shown in FIG. Circular protrusion 7a and step 7b
is formed, and the first step part 7bK is made of a ceramic material having an η-opening or a high-resistance metal such as stainless steel, Hastelloy, Inconel, etc., and has a thickness equal to the height of the protruding part 7a. One surface of the disk-shaped spacer 11 is fixed. 5 as shown in FIGS. 3 and 4 on the end surface of the protrusion 7a of the fixed electrode rod 7 and the other surface of the spacer 11. Is the outer diameter appropriately larger than the outer diameter of the electrode rod 7? The coil part 9a has a cylindrical shape and has a slit of 12% in the axial direction. ) The $1 coil 9, which is made up of a connecting arm 9b and a second connecting arm 9c, has a semicircular connection formed at the ends of the first connecting arm 9b and the second connecting arm 9c. The coil part 9a is fixed through the part 1111I, the pole rod 7
It is installed in such a way that it is arranged in series with the other. At the end of the arm 2 connecting arm 9c of the brush 1 coil 9,
Approximately semicircular protrusion 13d and step 13fi%' on one end surface
The formed auxiliary electrode rod 13 is fixed to the fixed electrode rod 71f through the end surface of the protrusion 13fi so as to be arranged in series, and the end of the first connecting arm 9h is coated with an insulating material or a high Made of resistive metal, - face auxiliary electrode rod 1
The other end of the disk-shaped spacer 14 fixed to the stepped portion 13hK of No. 3 is fixed. A circular recess 15 is provided on the other end surface of the auxiliary electrode rod 13, 1l-1rt. A cylindrical spacer 16 having one end or a concave portion 15
It is fixed to the bottom of the box and stored concentrically. Spacer 1
6 and the other end surface of the auxiliary electrode rod 13, there is an electrode connecting portion to, 1 formed in a cylindrical shape with an appropriately smaller diameter than the inner diameter of the recess 15, as shown in FIGS. 3 and 5. , City, Pole Connection 10aO) Four first arm portions iob, 1ob, . . . extending radially outward from positions divided into four equal parts on the outer circumferential surface. Approximately 40 of each @1 @ end of part 10b or f-1 1 coil 9
Four coil parts 10c, 10c, . Four second arm parts 10d extend radially inward in parallel with the first arm part 10b of each frame. 10d, . . . from the end of each second arm portion 10d to the recessed portion 1.
5 and the outer diameter of the auxiliary electrode rod 13. Four electrode rod connection portions 10e110 curved in the same circumferential direction on the inside and outside.
The second coil consisting of e, ... ] 0 is the electrode connection part 1
0fi and each electrode rod connecting portion 1 108 are fixedly connected together. At the other end of the electrode connection part IQq171 in the second coil 10, the fixed electrode 5, which is formed in the shape of a disk and has approximately the same diameter as the second coil 10, is located at the center of its back surface (top surface in FIG. 3). The recess 17 provided in the At the inner end of each magnetic field generating part 1 of the first coil 9 (separated from the LC and fitted in a loop-like manner, and the electrode rod 8σ on the flexible side), the fixed electrode 5 and The movable side electrode 6 is formed into a disk shape with the same diameter,
It is fitted through a recess provided in the center of its back surface (lower surface in Figure 3). In FIG. 2, 19 is a metal bellows, 20 is an intermediate shield concentrically surrounding each electrode 5.6 and the first coil 9, and 21.21 is an auxiliary shield fixed to the inner surface of each metal end plate 3. be. Also, ] In the 2 Brush 3 diagram, 22 is the Brush 2 coil 10'? This is a ring-disc-shaped coil reinforcing member fitted with the auxiliary electrode rod 13Vr for reinforcement and support, and is made of high-resistance metal, etc., and the W and x coils 9 are also reinforced through similar coil reinforcing members (not shown). 23 is a notch provided at the other end of the auxiliary electrode rod 13, so that the first arm portion 10b of the second coil 10 and the auxiliary electrode rod 13 are directly electrically connected. This is to prevent this. The interruption of the main circuit 'llr flow by the vacuum interrupter of the first embodiment with the above configuration is caused by an arc generated between the electrodes 5.6 due to the opening of the electrodes 5.6, or by an arc generated between the electrodes 5.6 and 5.6. This process is completed when the current reaches a natural zero value or close to it and disappears as the current is sufficiently opened.
In addition to taking the axial magnetic field Hv on the vertical axis, both coils 9 and 1
The axial magnetic field curve caused by 0 is 1gAA, 'B
, and the axial magnetic field that combines both axial magnetic fields is expressed as m
'SK, '811 coil 9 is shown in Figure 6, denoted by c.
Since an axial magnetic field of substantially uniform strength is applied in the radial direction by the second coil 10 and the second coil 10, the arc spot is formed on both electrodes 5. It is diffused almost uniformly over the entire surface between the pairs of R. In addition, in the above-mentioned embodiment, @2 coils 10%'
Although we have described the case where it is placed on the back of the fixed side electrode 5,
For example, the movable side electrode 6
It may be placed on the back of the IC, lE1
Similarly, the coil 9 may be electrically connected to the electrode rod 8 and the like on the movable side 4 . In addition, the brush 1 coil 9 is not limited to the so-called one-turn type with 12 slits in the axial direction;
Number of divisions within a range less than the number of divisions of 0? It is good to have more. 11-1, the vacuum container 4 is not limited to the case where it is formed from one insulating cylinder made up of two insulating cylinders 1 and the metal end plate 3.3 that closes both ends of the cylinder; Of course, it may be formed from three or more insulating cylinders and two metal end plates that close both ends of the cylinders, or from a metal cylinder and insulating end plates that close both ends of the cylinders. As described above, the present invention has two electrodes in a vacuum container. A pair introduced so as to be able to approach and separate relatively to each other is mechanically provided so as to be able to be moved toward and away from each other via an electrode rod, and the pair ? A cylindrical first coil having an axial slit on the outer circumference Vr1 or 2N of the electrode is arranged concentrically, and a coil with a diameter smaller than that of the first coil and a circumference is placed on the back of one or the other electrode. A second coil having an annular shape with an increased number of divisions in the direction is arranged, and the first coil and the second coil have the same polarity and are electrically connected to one or the other electrode rod and electrode in order to generate a magnetic field. Since it is connected to a VC, there is a spot of arc that occurs between the electrodes when the circuit is cut off.
It is possible to uniformly diffuse the electric current over the entire surface of the QT surface, which in turn brings about effects such as the ability to efficiently increase the number of new customers.

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

箪1図はコイル外径の変化に対する軸方向磁界の径方向
の分布状態ケ表わした説明図、駆2図は 6 本発明に係る真空インタラプタの縦断面図、第3図は本
発明の要部の縦断面図、第4図および筆5図はそ几ぞれ
本発明の要部の平面図、第6図は本賢明の作用説明図で
ある。 4・・・真空容器、5.6・・・電極% 7.8・・・
電極棒、9°°°@】コイル、10パ・第2コイル、1
2・・・スリット。 7 第1図 第2図 7 1 1 ゛ 。 6 I
Figure 1 is an explanatory diagram showing the distribution state of the axial magnetic field in the radial direction with respect to changes in the outer diameter of the coil, Figure 2 is a vertical cross-sectional view of the vacuum interrupter according to the present invention, and Figure 3 is the main part of the present invention. 4 and 5 are plan views of essential parts of the present invention, respectively, and FIG. 6 is an explanatory diagram of the operation of the present invention. 4...Vacuum container, 5.6...Electrode% 7.8...
Electrode rod, 9°°°@] Coil, 10 pa/2nd coil, 1
2...Slit. 7 Figure 1 Figure 2 7 1 1 ゛. 6 I

Claims (1)

【特許請求の範囲】 il+  真空容器内に1対の電極を相対的に接近離反
自在に導入した対をな−r[極棒を介し機械的に接離自
在に設け、前記対lなす電極の外周に1または2以上の
軸方向スリットン有する円筒状の第1コイルケ同心配置
するとともIlr、前記いずれか一方または他方の電極
の背部tIcfjIc1コイルより小径にしてかつ周方
向の分割数を多くした環状の@2コイル!配置し。 前記第1コイルおよび第2コイルl同一極性の磁界を発
生すべくそれぞnいず几か一方または他方の電極棒と電
極とに電気的に接続してなる真空インタラプタ。 1211に2コイルの外径ケ第1コイルの外径の40〜
70%としてなる特許請求の範囲第1′qi記載の真空
インタラプタ。
[Scope of Claims] il+ A pair of electrodes introduced into a vacuum container such that they can be moved relatively toward and away from each other. A cylindrical first coil having one or more axial slits on the outer periphery is arranged concentrically, and the back part of either one or the other electrode is an annular coil having a smaller diameter than the coil and having a larger number of circumferential divisions. @2 coils! Place. A vacuum interrupter in which the first coil and the second coil are electrically connected to one or the other electrode and an electrode in order to generate a magnetic field of the same polarity. 1211 is the outer diameter of the second coil.The outer diameter of the first coil is 40~
70%. Vacuum interrupter according to claim 1'qi.
JP16183382A 1982-09-17 1982-09-17 Vacuum interrupter Granted JPS5951427A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16183382A JPS5951427A (en) 1982-09-17 1982-09-17 Vacuum interrupter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16183382A JPS5951427A (en) 1982-09-17 1982-09-17 Vacuum interrupter

Publications (2)

Publication Number Publication Date
JPS5951427A true JPS5951427A (en) 1984-03-24
JPS6319054B2 JPS6319054B2 (en) 1988-04-21

Family

ID=15742787

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16183382A Granted JPS5951427A (en) 1982-09-17 1982-09-17 Vacuum interrupter

Country Status (1)

Country Link
JP (1) JPS5951427A (en)

Also Published As

Publication number Publication date
JPS6319054B2 (en) 1988-04-21

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