JPS5847630Y2 - Vacuum cutter - Google Patents

Vacuum cutter

Info

Publication number
JPS5847630Y2
JPS5847630Y2 JP9631579U JP9631579U JPS5847630Y2 JP S5847630 Y2 JPS5847630 Y2 JP S5847630Y2 JP 9631579 U JP9631579 U JP 9631579U JP 9631579 U JP9631579 U JP 9631579U JP S5847630 Y2 JPS5847630 Y2 JP S5847630Y2
Authority
JP
Japan
Prior art keywords
electrode
coil
current
tip
vacuum breaker
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
JP9631579U
Other languages
Japanese (ja)
Other versions
JPS5614438U (en
Inventor
泰司 野田
幸男 小針
誠治 石塚
秀水 川口
Original Assignee
株式会社明電舎
株式会社ゼムバツク
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 株式会社明電舎, 株式会社ゼムバツク filed Critical 株式会社明電舎
Priority to JP9631579U priority Critical patent/JPS5847630Y2/en
Publication of JPS5614438U publication Critical patent/JPS5614438U/ja
Application granted granted Critical
Publication of JPS5847630Y2 publication Critical patent/JPS5847630Y2/en
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は真空しゃ断器に関するものである。[Detailed explanation of the idea] The present invention relates to a vacuum breaker.

一般に真空しゃ断器は真空容器内に固定電極と可動電極
を対向配置して構成され、可動電極を固定電極に対して
接離することにより電流の投入。
Generally, a vacuum breaker is constructed by arranging a fixed electrode and a movable electrode facing each other in a vacuum container, and current is applied by moving the movable electrode toward and away from the fixed electrode.

しゃ断を行っている。It is shutting off.

しかるにしゃ断時には電極間にアークが発生し、このア
ークはしゃ断電流が大きいとアーク自身により生じた磁
界と外部回路の作る磁界との相互作用により電極外周方
向への電磁力を受け、アークは電極の外周部に片寄って
その部分を局部的に加熱し、多量の金属蒸気を発生させ
る。
However, when breaking, an arc is generated between the electrodes, and if the breaking current is large, this arc receives electromagnetic force in the direction of the electrode's outer circumference due to the interaction between the magnetic field generated by the arc itself and the magnetic field created by the external circuit, and the arc It leans toward the outer periphery and locally heats that area, generating a large amount of metal vapor.

このため、電流零点後に電極間に金属蒸気が残留し、絶
縁回復が遅れてしゃ断能力が低下する。
For this reason, metal vapor remains between the electrodes after the current reaches zero, delaying insulation recovery and reducing the breaking ability.

この対策として従来、アークに軸方向の磁界を印加する
ことが行われている。
Conventionally, as a countermeasure against this problem, applying an axial magnetic field to the arc has been carried out.

その一例を第1図に示す。An example is shown in FIG.

図において、1は絶縁筒、2,3は絶縁筒1の両端に取
付けられた端板、4は端板2に挿着された固定電極棒、
5は端板3に挿通されるとともにベローズ6を介して端
板3に取付けられた固定電極棒、7,8は夫々電極棒4
,5の先端に取付けられた固定電極および可動電極で、
可動電極8は基部9aを可動電極棒5の先端に取付けら
れるとともに基部9aからコイル状に伸びて一ターンコ
イルを形成するコイル部9bを有するコイル電極と、基
部9aにステンレス鋼などの高抵抗材10を介して取付
けられた接触電極11と、コイル部9bの先端と接触電
極11とを接続する接続導体12とから構成され、固定
電極7も同様にしてコイル電極13、高抵抗材14.接
触電極15および接続導体16とから構成される。
In the figure, 1 is an insulating tube, 2 and 3 are end plates attached to both ends of the insulating tube 1, 4 is a fixed electrode rod inserted into the end plate 2,
5 is a fixed electrode rod inserted into the end plate 3 and attached to the end plate 3 via a bellows 6; 7 and 8 are electrode rods 4, respectively;
, 5, with a fixed electrode and a movable electrode attached to the tip.
The movable electrode 8 is a coil electrode having a base 9a attached to the tip of the movable electrode rod 5, and a coil portion 9b that extends from the base 9a in a coil shape to form a one-turn coil, and the base 9a is made of a high resistance material such as stainless steel. 10, and a connecting conductor 12 that connects the tip of the coil portion 9b to the contact electrode 11. Similarly, the fixed electrode 7 includes a coil electrode 13, a high resistance material 14. It is composed of a contact electrode 15 and a connecting conductor 16.

この真空しゃ断器ではしゃ断時にしゃ断電流は例えば可
動電極棒5−コイル電極9−接続導体12−接触電極1
1−アーク−接触電極15−接続導体16−コイル電極
13−固定電極棒4の経路で流れ、各コイル電極9,1
3は軸方向磁界を発生する。
In this vacuum breaker, the breaking current at the time of breaking is, for example, movable electrode rod 5 - coil electrode 9 - connecting conductor 12 - contact electrode 1
1-Arc-contact electrode 15-Connecting conductor 16-Coil electrode 13-Fixed electrode rod 4 flow, each coil electrode 9,1
3 generates an axial magnetic field.

このため、アーク電流を運ぶ電子およびイオンなどの荷
電粒子がこの磁界に捕捉されてアークの集中は妨げられ
、各接触電極11.15は局部的に加熱されることがな
いので多量の金属蒸気を発生せず、電流零点後の絶縁回
復が早ます、シや断能力が向上する。
For this reason, charged particles such as electrons and ions carrying the arc current are captured by this magnetic field, preventing the concentration of the arc, and each contact electrode 11.15 is not locally heated, so a large amount of metal vapor is generated. This does not occur, and the insulation recovery after the current zero point is accelerated, and the breaking capacity is improved.

しかるに上記の真空しゃ断器ではコイル部9bは一ター
ンコイルを形成するため長さが長く、シかもコイル部9
bには投入状態では常時電流が流れるため熱損失が大き
く、大定格電流用の真空しゃ断器では温度上昇の不利が
ある。
However, in the above-mentioned vacuum breaker, the coil portion 9b is long because it forms a one-turn coil.
Since current always flows through b in the closed state, heat loss is large, and a vacuum breaker for large current ratings has the disadvantage of temperature rise.

又、従来ではコイル電極17を第2図に示すように分流
式にしたものがある。
Also, in the past, there is a coil electrode 17 of a shunt type as shown in FIG.

この場合、コイル電極17は基部17 aからコイル状
に伸びる士ターンのコイルを形成する4個のコイル部1
7bを有しており、各コイル部17 bの先端は夫々接
続導体18を介して接触電極と接続される。
In this case, the coil electrode 17 has four coil parts 1 forming a two-turn coil extending in a coil shape from the base part 17a.
7b, and the tip of each coil portion 17b is connected to a contact electrode via a connecting conductor 18, respectively.

この例では電極棒から基部17 aに流入した電流は各
コイル部17bに分流するため、各コイル部17bを流
れる電流は全電流の圭づつとなり、熱損失は小さくなる
が、軸方向磁界の大きさが小さくなる欠点がある。
In this example, the current flowing from the electrode rod to the base 17a is divided into each coil part 17b, so the current flowing through each coil part 17b is equal to one part of the total current, and heat loss is small, but the axial magnetic field is large. It has the disadvantage that it becomes smaller.

本考案は上記の点を考慮して、比較的大きな軸方向磁界
を発生することができるとともに熱損失が少く、かつ構
造簡単な真空しゃ断器を提供することを目的とする。
In consideration of the above points, it is an object of the present invention to provide a vacuum breaker that can generate a relatively large axial magnetic field, has low heat loss, and has a simple structure.

以下本考案の実施例を図面とともに説明する。Embodiments of the present invention will be described below with reference to the drawings.

第3図において、19は基部19 bを電極棒20の先
端に取付けられるとともに基部19 aに取付けられて
コイル状に伸び一ターンコイルを形成するコイル部19
bを有するコイル電極、21〜24は夫々コイル部1
9bに立設された接続導体で、各接続導体21〜24は
コイル部19 bの先端に近い位置に立設したものほど
径を大きくする。
In FIG. 3, reference numeral 19 denotes a coil portion 19 whose base portion 19 b is attached to the tip of the electrode rod 20 and which is attached to the base portion 19 a and extends into a coil to form a one-turn coil.
Coil electrodes 21 to 24 each have a coil part 1
The diameter of each of the connecting conductors 21 to 24 is increased as the connection conductor is erected at a position closer to the tip of the coil portion 19b.

25は各接続導体21〜24の先端に取付けられた接触
電極で、接触電極25にはその周辺部を四つの部片25
a〜25 dに仕切るとともにうず電流を抑制するた
めのスリツ) 25 eを放射状に設ける。
Reference numeral 25 denotes a contact electrode attached to the tip of each of the connecting conductors 21 to 24, and the contact electrode 25 has four pieces 25 attached to its periphery.
Slits (25) and 25e are provided radially to partition into sections a to 25d and to suppress eddy currents.

この真空しゃ断器では例えば電流は電極棒20から基部
19 aを介してコイル部19 bに流れる。
In this vacuum breaker, for example, current flows from the electrode rod 20 to the coil portion 19b via the base portion 19a.

次に電流は接続導体21〜23を介して夫々部片25b
〜25 dに次々の分流するためコイル部19 bを流
れる電流は次第に減少し、最後に接続導体24を介して
部片25 aに流れる。
The current then flows through the connecting conductors 21 to 23 to the respective parts 25b.
25d, the current flowing through the coil part 19b gradually decreases and finally flows through the connecting conductor 24 to the part 25a.

この際、仮に各接続導体21〜24の径が同じであれば
ほとんどの電流は接続導体21を通って流れ、接続導体
24を通って流れる電流はほとんど無しになる。
At this time, if the connecting conductors 21 to 24 have the same diameter, most of the current will flow through the connecting conductor 21, and almost no current will flow through the connecting conductor 24.

しかし、各接続導体21〜24はコイル部19bの基部
19 aに近い位置に立設したものほど径が小さくなっ
ているため抵抗が大きく、各接続導体21〜24を通っ
て流れる電流は平均化される。
However, the closer the connecting conductors 21 to 24 are installed upright to the base 19a of the coil portion 19b, the smaller the diameter, and therefore the higher the resistance, and the current flowing through each of the connecting conductors 21 to 24 is averaged. be done.

従って、第1図に示した従来のものと比べるとコイル部
19 bを流れる電流が次第に減少するため熱損失は小
さくなり、しかしコイル部19 bを一ターン流れる電
流もあるため軸方向磁界はあまり小さくならない。
Therefore, compared to the conventional one shown in FIG. 1, the current flowing through the coil portion 19b gradually decreases, resulting in smaller heat loss. However, since some current flows through the coil portion 19b for one turn, the axial magnetic field is not large enough. It doesn't get smaller.

又、第2図に示した分流形のものと比べると熱損失は若
干大きくなるが、軸方向磁界は大幅に大きくすることが
できる。
Furthermore, although the heat loss is slightly greater than that of the shunt type shown in FIG. 2, the axial magnetic field can be significantly increased.

尚、電流が逆方向即ち接触電極25から各接続導体21
〜24を通ってコイル電極19に流れる際にも電流は各
接続導体21〜24を平均化して流れるため上記と同じ
効果がある。
Note that the current flows in the opposite direction, that is, from the contact electrode 25 to each connection conductor 21.
24 to the coil electrode 19, the current flows through each connecting conductor 21 to 24 in an average manner, so that the same effect as described above is obtained.

又、第3図に示した電極構造は固定、可動の両電極の双
方又は一方のみに適用することができる。
Further, the electrode structure shown in FIG. 3 can be applied to both or only one of fixed and movable electrodes.

以上のように本考案においては一ターンコイルを形成す
るコイル電極と接触電極との間に複数本の接続導体を設
け、この各接続導体の径はコイル電極の先端に近いもの
ほど大きくしている。
As described above, in the present invention, a plurality of connecting conductors are provided between the coil electrode and the contact electrode that form a one-turn coil, and the diameter of each connecting conductor increases as it approaches the tip of the coil electrode. .

このため、電流はコイル電極の基部に近い接続導体のみ
に流れるようなことはなく、各接続導体に平均化して流
れる。
Therefore, the current does not flow only to the connecting conductor near the base of the coil electrode, but flows in an average manner to each connecting conductor.

従って、コイル電極を一ターン流れる電流も存在し、従
来の一ターン形のコイル電極を有するものに比べて軸方
向磁界の大きさはあまり減少せず、大きなしゃ断能力を
有する。
Therefore, there is also a current that flows through the coil electrode for one turn, and the magnitude of the axial magnetic field does not decrease much compared to the conventional one-turn type coil electrode, and it has a large blocking ability.

しかも、コイル電極を流れる電流は各接続導体への分流
により次第に減少するため熱損失は小さくなり、大定格
電流用の真空しゃ断器においても温度上昇の不利を生し
難くなる。
Furthermore, since the current flowing through the coil electrodes is gradually reduced by being shunted to each connected conductor, heat loss is reduced, and even in a vacuum breaker for a large rated current, the disadvantage of temperature rise is less likely to occur.

又、各接続導体がコイル電極と接触電極の間のスペーサ
ともなるので従来のように高抵抗材から戒る特別のスペ
ーサを設ける必要がなく、構造簡単となる。
In addition, since each connecting conductor also serves as a spacer between the coil electrode and the contact electrode, there is no need to provide a special spacer that requires high resistance materials as in the prior art, and the structure is simplified.

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

第1図A、Bは夫々従来の真空しゃ断器の縦断正面図お
よびコイル電極の斜視図、第2図は従来の他の真空しゃ
断器の斜視図、第3図A、Bは夫々本考案に係る真空し
ゃ断器の電極部分の正面図および電極部分の分解斜視図
。 1・・・・・・絶縁筒、2,3・・・・・・端板、6・
・・・・・ベローズ、19・・・・・・コイル電極、2
0・・・・・・電極棒、21〜24・・・・・・接続導
体、25・・・・・・接触電極。
Figures 1A and B are a longitudinal sectional front view and a perspective view of a coil electrode of a conventional vacuum breaker, respectively, Figure 2 is a perspective view of another conventional vacuum breaker, and Figures 3A and B are respectively related to the present invention. FIG. 2 is a front view and an exploded perspective view of an electrode portion of such a vacuum breaker. 1... Insulating cylinder, 2, 3... End plate, 6.
...Bellows, 19...Coil electrode, 2
0... Electrode rod, 21-24... Connection conductor, 25... Contact electrode.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 真空容器内に夫々電極棒を介して一対の電極を接離可能
に対向配置した真空しゃ断器において、電極棒の先端に
取付けられるとともに軸方向磁界を発生する一ターンコ
イルを形成するコイル電極と、コイル電極に立設される
とともに立設位置がコイル電極の先端に近いものほど径
を大きくされた複数本の接続導体と、各接続導体の先端
に取付けられた接触電極とから少くとも一方の電極を構
成したことを特徴とする真空しゃ断器。
In a vacuum breaker in which a pair of electrodes are arranged facing each other so as to be able to come into contact with and be separated from them through electrode rods in a vacuum container, a coil electrode that is attached to the tip of the electrode rod and forms a one-turn coil that generates an axial magnetic field; At least one of the plurality of connection conductors that are erected on the coil electrode and whose diameter increases as the erected position is closer to the tip of the coil electrode, and a contact electrode attached to the tip of each connection conductor. A vacuum breaker characterized by comprising:
JP9631579U 1979-07-12 1979-07-12 Vacuum cutter Expired JPS5847630Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9631579U JPS5847630Y2 (en) 1979-07-12 1979-07-12 Vacuum cutter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9631579U JPS5847630Y2 (en) 1979-07-12 1979-07-12 Vacuum cutter

Publications (2)

Publication Number Publication Date
JPS5614438U JPS5614438U (en) 1981-02-07
JPS5847630Y2 true JPS5847630Y2 (en) 1983-10-31

Family

ID=29329145

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9631579U Expired JPS5847630Y2 (en) 1979-07-12 1979-07-12 Vacuum cutter

Country Status (1)

Country Link
JP (1) JPS5847630Y2 (en)

Also Published As

Publication number Publication date
JPS5614438U (en) 1981-02-07

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