JPS6319054B2 - - Google Patents

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Publication number
JPS6319054B2
JPS6319054B2 JP16183382A JP16183382A JPS6319054B2 JP S6319054 B2 JPS6319054 B2 JP S6319054B2 JP 16183382 A JP16183382 A JP 16183382A JP 16183382 A JP16183382 A JP 16183382A JP S6319054 B2 JPS6319054 B2 JP S6319054B2
Authority
JP
Japan
Prior art keywords
coil
electrode
magnetic field
outer diameter
axial magnetic
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.)
Expired
Application number
JP16183382A
Other languages
Japanese (ja)
Other versions
JPS5951427A (en
Inventor
Takamitsu Sano
Hideo Kawakami
Takashi Ashizawa
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 Electric Manufacturing Co Ltd
Original Assignee
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 Electric Manufacturing Co Ltd filed Critical Meidensha Electric Manufacturing Co Ltd
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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Description

【発明の詳細な説明】 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を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。
DETAILED DESCRIPTION OF THE INVENTION 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.

従来、軸方向の磁界(縦磁界)を発生させる手
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口部を両端
に固着した封着金具を介し金属端板により閉塞し
かつ内部を高真空に排気して真空容器を形成し、
この真空容器内に円板状をなす1対の電極を各金
属端板の中央から相対的に接近離反自在に導入し
た対をなす電極棒を介し機械的に接触離反(接
離)自在に設けるとともに、各電極とそれぞれの
電極棒とを同一極性の軸方向磁界を発生すべくそ
れぞれの電極の背部に配置した有端環状または周
方向へ2以上に分割された環状にしてかつ電極と
ほぼ同外径のコイルを介し電気的に直列接続して
構成されている。
Conventionally, a vacuum interrupter that is equipped with a means for generating an axial magnetic field (vertical magnetic field) around an electrode is usually made of glass or the like by connecting both openings of an insulating cylinder to a metal end plate through sealing fittings fixed to both ends. to close the container and evacuate the inside to a high vacuum to form a vacuum container,
A pair of disk-shaped electrodes are provided in this vacuum container so that they can be mechanically brought into contact with and separated from each other through a pair of electrode rods that are introduced from the center of each metal end plate so that they can approach and separate from each other. In addition, each electrode and each electrode rod are arranged in the back of each electrode in order to generate an axial magnetic field of the same polarity, and are arranged in the shape of an end ring or in the form of a ring divided into two or more parts in the circumferential direction, and are substantially the same as the electrodes. They are electrically connected in series via a coil with an outer diameter.

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、電極の接離により生ずるアークを
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、もつてしや断容量を径方向(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ツトが、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
たはその中心を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。
However, conventional axial magnetic field type vacuum interrupters use an axial magnetic field to confine the arc generated by the contact and separation of the electrodes in the space between the electrodes to stabilize it, and to reduce the radial (transverse) magnetic field. Although it can be increased more than that of the method,
There is a problem in that the arc spots on the electrode surface are not scattered near the outer periphery of the electrode and are concentrated and unevenly distributed near the center or on concentric circles around the center, making it impossible to utilize the electrode surface effectively. .

かかる現象は、同一極性の磁界を発生する2個
のコイルを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を変化させて、両コイル
による合成された軸方向磁界の径方向の分布状態
を測定した実験結果を示す第1図からも明らかな
如く、合成された軸方向磁界の径方向の分布状態
が不均一であることに依ると思われる。すなわ
ち、第1図は横軸にコイルの外径Rを、縦軸に合
成された軸方向磁界の強度Hをとり、コイルの外
径Rを変化させた場合の合成された軸方向磁界の
径方向の分布状態を、コイルの外径Rの増大の順
に曲線A,B,CおよびDで示したもので、これ
によればコイルの外径Rが小さい場合には、曲線
Aで示すように、合成軸方向磁界の強度Hがコイ
ルの中心Oにおいて最高となる凸状を呈し、また
コイルの外径Rが大きい場合には、曲線B,Cお
よびDで示すように、合成軸方向磁界の強度Hが
コイルの中心Oに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を呈するとと
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、合成軸方向磁
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、アークスポツトの偏在を招来し
ていることが判るものである。
This phenomenon is achieved by separating two coils that generate magnetic fields of the same polarity by a predetermined distance in the axial direction, and
As is clear from Figure 1, which shows the experimental results of measuring the radial distribution state of the combined axial magnetic field from both coils by keeping both coils the same and changing their outer diameters, the combined axial magnetic field This seems to be due to the non-uniform distribution state in the radial direction. In other words, in Figure 1, the horizontal axis is the outer diameter R of the coil, and the vertical axis is the intensity H of the combined axial magnetic field, and the diameter of the combined axial magnetic field when the outer diameter R of the coil is changed. The distribution state of the direction is shown by curves A, B, C, and D in the order of increasing outer diameter R of the coil. According to this, when the outer diameter R of the coil is small, as shown by curve A , when the strength H of the composite axial magnetic field is the highest at the center O of the coil, and when the outer diameter R of the coil is large, the strength H of the composite axial magnetic field is as shown by curves B, C, and D. The strength H is lowest at the center O of the coil and highest near the inner circumference of the coil, forming a concave shape, and as the outer diameter R of the coil increases, the lowest and highest points tend to decrease, and the resultant axial magnetic field In other words, it can be seen that uneven distribution of arc spots is caused by uneven distribution of magnetic flux density in the radial direction.

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、対をなす電極棒を
介して真空容器内において機械的に接離自在に設
けられる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ツトを
有する円筒状の第1コイルを同心配置するととも
に、いずれか一方または他方の電極の背部に凸状
にしてかつ第1コイルより強度の小さい軸方向磁
界を発生すべく第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コイルを同心
配置し、これらの第1コイルおよび第2コイルを
同一極性の磁界を発生すべくそれぞれいずれか一
方または他方の電極棒と電極とに電気的に接続す
ることにより、両コイルによる合成軸方向磁界の
径方向の分布状態を電極面全面に亘つて均一にし
てアークスポツトの均一な拡散を図り、もつて電
極面を有効に活用し得るようにした軸方向磁界方
式の真空インタラプタを提供するにある。以下、
第2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 form a concave shape on the outer periphery of a pair of electrodes that are mechanically provided in a vacuum container so as to be freely accessible and detachable through a pair of electrode rods. A first cylindrical coil having one or more axial slits is arranged concentrically in order to generate an axial magnetic field of In order to generate a low-strength axial magnetic field, a second annular coil with a smaller diameter than the first coil and a larger number of circumferential divisions is arranged concentrically, and these first and second coils are connected to a magnetic field of the same polarity. By electrically connecting one or the other electrode to the electrode, the radial distribution of the combined axial magnetic field from both coils is made uniform over the entire surface of the electrode, thereby creating an arc spot. An object of the present invention is to provide an axial magnetic field type vacuum interrupter which is capable of uniformly dispersing the magnetic field and making effective use of the electrode surface. below,
Embodiments of the present invention will be described in detail with reference to FIG. 2 and subsequent drawings.

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
したガラス、セラミツクス等からなる2本の絶縁
筒1,1,を、両端に固着したコバール等からな
る薄肉円環状の封着金具2,2,…の一方を介し
て同軸的に接合して1本の絶縁筒とするととも
に、その両開口部を他方の封着金具2,2を介し
ステンレス鋼等から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を形成し、この真空容器4内にほぼ同外径
の円板状をなす1対の電極5,6を各金属端板
3,3の中央部から真空容器4の気密性を保持し
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を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)のスリツトを有する円筒状の
第1コイル9を同心配置するとともに、第1コイ
ル9と相俟つて電極5,6間における径方向(第
2図において左右方向)の磁界分布を均一にすべ
く、固定側(第2図において上側)の電極5の背
部にこの電極5と同径にしてかつ円周方向の分割
数を第1コイル9より多くした環状の第2コイル
10を固定側電極棒7に対して同心配置し、第1
コイル9および第2コイル10を同一極性の軸方
向磁界を発生すべくそれぞれ固定側電極棒7と固
定側電極5とに電気的に接続して概略構成されて
いる。
FIG. 2 is a longitudinal sectional view of a vacuum interrupter according to the present invention. This vacuum interrupter consists of two cylindrical insulating cylinders 1, 1 made of glass, ceramics, etc., made of Kovar etc. fixed to both ends. are coaxially joined through one of the thin-walled annular sealing fittings 2, 2, . Disc-shaped metal end plates 3, 3 consisting of etc.
A vacuum container 4 is formed by closing the interior with a high vacuum and evacuating the inside to a high vacuum. Inside this vacuum container 4, a pair of disk-shaped electrodes 5 and 6 having approximately the same outer diameter are attached to each metal end plate 3, A pair of electrode rods 7 and 8 are introduced from the center of the vacuum container 4 so as to be able to approach and separate from each other while maintaining the airtightness of the vacuum vessel 4. A cylindrical first coil 9 having a slit in the axial direction (vertical direction in FIG. 2) is arranged concentrically on the outer circumference of the electrodes 5 and 6, and together with the first coil 9, the radial direction ( In order to make the magnetic field distribution uniform in the horizontal direction (in the left-right direction in Fig. 2), a first coil is installed on the back of the electrode 5 on the fixed side (the upper side in Fig. 2) with the same diameter as this electrode 5 and the number of divisions in the circumferential direction. The number of annular second coils 10 larger than 9 is arranged concentrically with respect to the fixed electrode rod 7, and the first
The coil 9 and the second coil 10 are electrically connected to the fixed electrode rod 7 and the fixed electrode 5, respectively, to generate axial magnetic fields of the same polarity.

すなわち、固定側電極棒7の内端面には、第3
図に示すように、ほぼ半円形の突出部7aと段部
7bが形成されており、段部7bには、セラミツ
クスの如き絶縁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を有する円板状の
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1
1の他面には、第3図および第4図に示すよう
に、電極棒7の外径より適宜大きい外径を有する
円筒形にしてかつ軸方向のスリツト12を有する
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)からスリツト12を間にして
半径方向(第2図において左右方向)内方へ平行
に延伸した第1接続腕9bおよび第2接続腕9c
とからなる前記第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を固定側電極棒7に対
し直列配置となるが如くして取付けられている。
That is, on the inner end surface of the fixed electrode rod 7, there is a third
As shown in the figure, a substantially semicircular protrusion 7a and a stepped portion 7b are formed, and the stepped portion 7b is made of an insulating material such as ceramics or a high-resistance metal such as stainless steel, Hastelloy, Inconel, etc. ,
One surface of a disk-shaped spacer 11 having a thickness equivalent to the height of the protrusion 7a is fixed. and,
The end face of the protrusion 7a of the fixed electrode rod 7 and the spacer 1
As shown in FIGS. 3 and 4, the other surface of the 1 has a cylindrical coil portion 9a having an outer diameter suitably larger than the outer diameter of the electrode rod 7 and has an axial slit 12, and a coil portion 9a. A first connecting arm 9b and a second connecting arm 9c extend parallel to each other in the radial direction (left-right direction in FIG. 2) inward from one cylindrical end (upper end in FIG. 3) of the portion 9a with the slit 12 in between.
The first coil 9 consisting of the first connecting arm 9b
The coil portion 9a is attached to the stationary electrode rod 7 in series through a semicircular connection portion formed at the end of the second connection arm 9c.

前記第1コイル9における第2接続腕9cの端
部には、一端面にほぼ半円形の突出部13aと段
部13bを形成した補助電極棒13が、固定側電
極棒7に対し直列配置となるが如くし突出部13
aの端面を介して固着されているとともに、第1
接続腕9bの端部には、絶縁物または高抵抗の金
属からなり、一面を補助電極棒13の段部13b
に固着した円板状のスペーサ14の他面が固着さ
れている。補助電極棒13の他端面には、円形の
凹部15が設けられており、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を有する円筒状のスペーサ
16が、一端を凹部15の底部に固着して同心状
に収納されている。スペーサ16の他端および補
助電極棒13の他端面には、第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
に形成した電極接続部10aと、電極接続10a
の外周面における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10b,10b,…
と、各第1腕部10bの端部から第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1/4周ずつ同一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の端部からそれぞれの第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10
d,10d,…と、各第2腕部10dの端部から
凹部15の内径および補助電極棒13の外径を
内,外径としてほぼ1/4周ずつ各コイル部10c
とは反対の同一円周方向へ彎曲した4個の電極棒
接続部10e,10e,…とからなる前記第2コ
イル10が、電極接続部10aおよび各電極棒接
続部10eの一端を介して固着されている。そし
て、第2コイル10における電極接続部10aの
他端には、第2コイル10とほぼ同径の円板状に
形成された前記固定側の電極5が、その背面(第
3図において上面)中央に設けた凹部17を介し
第1コイル9の各磁界発生部10cから離隔され
るが如くして嵌着されており、また、可動側の電
極棒8の内端には、固定側の電極5と同径の円板
状に形成された前記可動側の電極6が、その背面
(第3図において下面)中央に設けた凹部18を
介して嵌着されている。
At the end of the second connecting arm 9c of the first coil 9, an auxiliary electrode rod 13 having a substantially semicircular protrusion 13a and a step 13b formed on one end surface is arranged in series with the stationary electrode rod 7. Narugashi protrusion 13
is fixed via the end face of a, and the first
The end of the connecting arm 9b is made of an insulating material or a high-resistance metal, and one side is connected to the stepped portion 13b of the auxiliary electrode rod 13.
The other surface of the disc-shaped spacer 14 is fixed to the spacer. A circular recess 15 is provided on the other end surface of the auxiliary electrode rod 13.
The recess 15 is made of an insulating material or a high-resistance metal.
A cylindrical spacer 16 having a length comparable to the depth is concentrically housed with one end fixed to the bottom of the recess 15 . At the other end of the spacer 16 and the other end surface of the auxiliary electrode rod 13, as shown in FIG. 3 and FIG.
Four first arm portions 10b, 10b, . . . extend radially outward from positions divided into four equal parts on the outer circumferential surface of
and 4 curved in the same circumferential direction from the end of each first arm portion 10b by approximately 1/4 turn with a radius of curvature of approximately 40 to 70% (approximately 60% in this embodiment) of the first coil 9.
four second arm parts 10 extending radially inward from the end of each coil part 10c parallel to each first arm part 10b.
d, 10d, ..., each coil part 10c is approximately 1/4 circumference from the end of each second arm part 10d with the inner diameter of the recess 15 and the outer diameter of the auxiliary electrode rod 13 as the inner and outer diameters.
The second coil 10, which is made up of four electrode rod connecting portions 10e, 10e, . has been done. At the other end of the electrode connection part 10a of the second coil 10, the fixed side electrode 5, which is formed in the shape of a disk having approximately the same diameter as the second coil 10, is attached to its back surface (top surface in FIG. 3). The first coil 9 is fitted so as to be spaced apart from each magnetic field generating section 10c through a recess 17 provided in the center, and the fixed electrode is attached to the inner end of the movable electrode rod 8. The movable side electrode 6 formed in the shape of a disk having the same diameter as the movable side electrode 6 is fitted through a recess 18 provided at the center of its back surface (lower surface in FIG. 3).

なお、第2図において19は金属ベローズ、2
0は各電極5,6および第1コイル9等を同心状
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、第3図において22は第2コイル10を補助
支持すべく補助電極棒13に嵌着したリング円板
状のコイル補助部材で、高抵抗の金属等からなる
ものであるとともに、第1コイル9も図示しない
同様のコイル補助部材を介して補助支持されてい
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するのを防
止するためのものである。
In addition, in FIG. 2, 19 is a metal bellows;
0 is an intermediate shield concentrically surrounding each electrode 5, 6, first coil 9, etc., and 21, 21 is an auxiliary shield fixed to the inner surface of each metal end plate 3. Further, in FIG. 3, reference numeral 22 denotes a ring-disc-shaped coil auxiliary member fitted onto the auxiliary electrode rod 13 to support the second coil 10, and is made of a high-resistance metal or the like. 9 is also auxiliary supported via a similar coil auxiliary member (not shown), and 23 is a notch provided at the other end of the auxiliary electrode rod 13, which connects the first arm portion 10b of the second coil 10 and the auxiliary electrode rod. This is to prevent direct electrical continuity with 13.

以上の構成の第1実施例の真空インタラプタに
よる主回路電流のしや断は、通常の真空インタラ
プタと同様に、電極5,6の開離によつて両者間
に生じたアークが、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つ
て消滅することにより完了するものであるが、電
極5,6間に発生したアークは、横軸にコイル外
径R、縦軸に軸方向磁界Hをとるとともに、両コ
イル9,10により生ずる軸方向磁界を曲線A,
Bで示し、また両軸方向磁界を合成した軸方向磁
界を曲線Cで表わした第6図に示すように、第1
コイル9と第2コイル10とにより径方向に亘つ
てほぼ均一な強さの軸方向磁界が印加されること
になるので、そのアークスポツトが両電極5,6
の対向する面全面に亘りほぼ均一に拡散されるも
のである。
The interruption of the main circuit current by the vacuum interrupter of the first embodiment having the above configuration is similar to that of a normal vacuum interrupter. The arc generated between the electrodes 5 and 6 is completed when electrodes 5 and 6 are sufficiently opened and the current reaches or near a natural zero value and disappears. In addition to taking an axial magnetic field H on the shaft, the axial magnetic field generated by both coils 9 and 10 is expressed by a curve A,
As shown in FIG.
Since an axial magnetic field of substantially uniform strength is applied in the radial direction by the coil 9 and the second coil 10, the arc spot is applied to both electrodes 5 and 6.
It is diffused almost uniformly over the entire surface facing each other.

なお、上述した実施例においては、第2コイル
10を固定側電極5の背部に配置した場合につい
て述べたが、これに限定されるものではなく、た
とえば可動側電極6の背部に配置してもよいもの
であるとともに、第1コイル9も同様に、可動側
の電極棒8等と電気的に接続してもよいものであ
る。また、第1コイル9は軸方向のスリツト12
を1個設けたいわゆる1ターンタイプのものに限
らず、第2コイル10の分割数より少ない範囲内
において分割数を多くしてもよいものである。さ
らに、真空容器4は、2本の絶縁筒1からなる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を閉塞する2枚の
金属端板とから形成したり、金属筒とその両端を
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。
In addition, in the above-mentioned embodiment, the case where the second coil 10 is arranged on the back of the fixed side electrode 5 has been described, but the invention is not limited to this, and for example, the second coil 10 may be arranged on the back of the movable side electrode 6. In addition to being good, the first coil 9 may also be electrically connected to the movable electrode rod 8 and the like. Further, the first coil 9 has an axial slit 12.
It is not limited to the so-called one-turn type in which one coil is provided, but the number of divisions may be increased within a range smaller than the number of divisions of the second coil 10. Furthermore, the vacuum container 4 is made up of two insulating cylinders 1.
The insulating cylinder of the book and metal end plates 3, 3 that close both ends of the book
For example, it may be formed from one or more insulating tubes and two metal end plates that close both ends of the insulating tube, or it may be formed from a metal tube and an insulating end plate that closes both ends of the insulating tube. Of course, it may be formed.

以上の如く本発明は、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す電極
棒を介し機械的に接離自在に設け、前記対をなす
電極の外周に1または2以上の軸方向スリツトを
有する円筒状の第1コイルを同心配置するととも
に、前記いずれか一方または他方の電極の背部に
第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コイルを配置し、前記第1コ
イルおよび第2コイルを同一極性の磁界を発生す
べくそれぞれいずれか一方または他方の電極棒と
電極とに電気的に接続したものであるから、しや
断時に電極間に発生するアークのスポツトを電極
面全面に亘り均一に拡散することができ、ひいて
はしや断容量を効率よく増大することができる等
の効果を奏する。
As described above, the present invention provides a pair of electrodes that are mechanically provided in a vacuum container so that they can be moved toward and away from each other through a pair of electrode rods that are introduced into a vacuum container so as to be able to move toward and away from each other. Alternatively, a cylindrical first coil having two or more axial slits is arranged concentrically, and an annular coil having a smaller diameter than the first coil and a larger number of circumferential divisions is placed on the back of one or the other electrode. A second coil is arranged, and the first coil and the second coil are electrically connected to one or the other electrode and electrode in order to generate a magnetic field of the same polarity. The arc spots that sometimes occur between the electrodes can be uniformly diffused over the entire surface of the electrodes, resulting in effects such as the ability to efficiently increase the capacitance and capacity.

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

第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を表わした説明図、第2図は
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図および第5
図はそれぞれ本発明の要部の平面図、第6図は本
発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…第1コイル、10…第2コイル、12…
スリツト。
FIG. 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, FIG. 2 is a longitudinal cross-sectional view of the vacuum interrupter according to the present invention, and FIG.
The figures are longitudinal cross-sectional views of the main parts of the present invention, Figures 4 and 5.
Each figure is a plan view of the main part of the present invention, 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... First coil, 10... Second coil, 12...
Slits.

Claims (1)

【特許請求の範囲】 1 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す電極棒を介し機械的に接
離自在に設け、前記対をなす電極の外周に1また
は2以上の軸方向スリツトを有する円筒状の第1
コイルを同心配置するとともに、前記いずれか一
方または他方の電極の背部に第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
コイルを配置し、前記第1コイルおよび第2コイ
ルを同一極性の磁界を発生すべくそれぞれいずれ
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。 2 第2コイルの外径を第1コイルの外径の40〜
70%としてなる特許請求の範囲第1項記載の真空
インタラプタ。
[Scope of Claims] 1. A pair of electrodes are provided in a vacuum container so as to be mechanically movable toward and away from each other through a pair of electrode rods introduced so as to be able to move toward and away from each other, and 1. or a cylindrical first having two or more axial slits.
The coils are arranged concentrically, and a second annular coil having a smaller diameter than the first coil and a larger number of divisions in the circumferential direction is provided on the back of one or the other electrode.
A vacuum interrupter in which a coil is arranged, and the first coil and the second coil are electrically connected to one or the other electrode rod and electrode, respectively, to generate a magnetic field of the same polarity. 2 Set the outer diameter of the second coil to 40 to the outer diameter of the first coil.
70% of the vacuum interrupter according to claim 1.
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 JPS5951427A (en) 1984-03-24
JPS6319054B2 true 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
JPS5951427A (en) 1984-03-24

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