JPS6122524A - Vacuum bulb - Google Patents

Vacuum bulb

Info

Publication number
JPS6122524A
JPS6122524A JP14220184A JP14220184A JPS6122524A JP S6122524 A JPS6122524 A JP S6122524A JP 14220184 A JP14220184 A JP 14220184A JP 14220184 A JP14220184 A JP 14220184A JP S6122524 A JPS6122524 A JP S6122524A
Authority
JP
Japan
Prior art keywords
magnetic field
electrode
vacuum
cylindrical conductor
electrodes
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
JP14220184A
Other languages
Japanese (ja)
Inventor
康一 安岡
邦夫 横倉
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP14220184A priority Critical patent/JPS6122524A/en
Publication of JPS6122524A publication Critical patent/JPS6122524A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の技術分野」 本発明は真空バルブ(=関する。[Detailed description of the invention] [Technical field of invention] The present invention relates to a vacuum valve.

〔発明の妖術的背景とその問題点〕[Magical background of invention and its problems]

従来の縦磁界を利用した真空バルブは真空中でのアーク
拡散性を有効(=利用して電流遮断を行わせるものであ
って、その一般的構成は第3図4二示す通りである。は
ぼ円筒状に形成された絶縁容器1とその両開口端を密封
する72ンジ2および3とで真空容器を形成しこの内部
(−7ランジ2.3を気密シニ貫通する固定側導電棒4
および可動側導電棒5の対向端に取付けられた固定電極
6および可mJ電極7が配置されている。固定電極6は
生電極6aおよびコイル電極6bから成っている。可動
電極7は生電極7aおよびコイル電極7bから成ってい
る。可動側導電棒5は7ランジ3C二対して気密を保ち
ながら図示していない駆動装置によシ軸方向(=駆動さ
れる。その気密性保持のため真空容器内において可動側
導電棒5と7ランジ3との間にベローズ8が配置されて
いる。コイル電極6b 。
A conventional vacuum valve using a vertical magnetic field effectively utilizes arc dispersion in a vacuum to interrupt current, and its general configuration is as shown in Fig. 3-42. A vacuum container is formed by an insulating container 1 formed into a substantially cylindrical shape and 72 flange 2 and 3 that seal both open ends of the insulating container 1.
A fixed electrode 6 and a mJ electrode 7 attached to opposite ends of the movable conductive rod 5 are arranged. The fixed electrode 6 consists of a live electrode 6a and a coil electrode 6b. The movable electrode 7 consists of a raw electrode 7a and a coil electrode 7b. The movable conductive rod 5 is driven in the axial direction by a drive device (not shown) while maintaining airtightness with respect to the 7 langes 3C.In order to maintain the airtightness, the movable conductive rods 5 and 7 are A bellows 8 is arranged between the flange 3 and the coil electrode 6b.

7bil:4流逍断の際C二、両生°緘極6a、7a間
に発生するアークと平行な縦磁界10を発生させる。コ
イA/電極6b、7bは縦磁界10を発生させるべく可
動側4#竜棒5の細心と直角な平向内で周方向に走るタ
ーンを形成している。縦磁界100強度および分布は、
・前記コイル電極形状、ターン数、また両主砲極間距離
によシ変化する。シールド9は電流遮断の際C二金属蒸
気が絶縁容器1に付着して真空パルブの耐圧低下や損傷
を生じたりする不具合を防止するため電極6.7を取シ
囲むように設けられている。
7bill: When four currents are transmitted, C2 generates a longitudinal magnetic field 10 parallel to the arc generated between the amphibious poles 6a and 7a. The coil A/electrodes 6b and 7b form a turn running in the circumferential direction in a plane perpendicular to the length of the movable side 4# dragon rod 5 to generate a vertical magnetic field 10. The longitudinal magnetic field 100 strength and distribution are:
・Varies depending on the shape of the coil electrode, the number of turns, and the distance between the two main gun poles. The shield 9 is provided so as to surround the electrodes 6.7 in order to prevent problems such as a decrease in the withstand voltage or damage to the vacuum valve due to the adhesion of C2 metal vapor to the insulating container 1 during current interruption.

ている。ing.

縦磁界を印加してアークの集中を防ぎ高い遮断性能を確
保しようとする真空バルブにおいては、充分な強度の磁
界を圧電極間(=有効に作用させるために圧電極の後方
近傍i二装置している。このため第4図に示すように主
電極間中央における磁界強度は、土電極弐面(=おける
磁界強度よ勺も低下し、土竜極間中央部で外側に脹らん
だ磁界分布となる。この傾向は主電極間距離に対するコ
イル電極径の比が小さくなるにつれて顕著となる。縦磁
界が電極間中央部で弱くなると、アーク電流を維持する
プ2ズマ粒子の拡散が増加しアーク電圧が上昇する。ア
ーク電圧が上昇すると電極への入力エネルギーが増すの
でアノードスポットが生じ易くなシ、電極消耗量の増加
、シールドの損傷増大ひいては、遮断不能にもつながる
In vacuum valves that apply a vertical magnetic field to prevent arc concentration and ensure high interrupting performance, a sufficiently strong magnetic field is applied between the piezo electrodes (i.e., in order to effectively act Therefore, as shown in Fig. 4, the magnetic field strength at the center between the main electrodes is lower than that at the second surface of the earth electrode, resulting in a magnetic field distribution that swells outward at the center between the two earth electrodes. This tendency becomes more pronounced as the ratio of the coil electrode diameter to the distance between the main electrodes becomes smaller.When the longitudinal magnetic field becomes weaker at the center between the electrodes, the diffusion of plasma particles that maintain the arc current increases, and the arc voltage increases. As the arc voltage increases, the energy input to the electrode increases, making it more likely that an anode spot will occur, leading to increased electrode wear, increased damage to the shield, and even failure to shut off.

このように磁界分布は真空バルブの寿命および遮断性能
に多大な影響を与えるためコイAIwL他形状電極配置
の決定(−際しては充分な検討が必要である。ところが
、形状の工夫による磁界分布の均一化にはおのずと限度
があ夛、とくに先に述べたよう(−主電極間距離に対す
るコイル電極径の比が小さい場合では、磁界分布を均一
にすることは困虐であった。
As described above, the magnetic field distribution has a great effect on the lifespan and cut-off performance of the vacuum valve, so it is necessary to carefully consider the arrangement of the electrodes of other shapes. There are naturally many limits to making the magnetic field uniform, and as mentioned above, it is especially difficult to make the magnetic field distribution uniform when the ratio of the coil electrode diameter to the distance between the main electrodes is small.

〔発明の目的〕[Purpose of the invention]

本発明は遮断性能(=優れ、しかも信頼性が高くかつ長
寿命の縦磁界方式の真空バルブを提供することを目的と
するものである。
An object of the present invention is to provide a vertical magnetic field type vacuum valve with excellent shutoff performance, high reliability, and long life.

〔発明の概要〕[Summary of the invention]

本発明は、電極の周囲に円筒導体を設け、!極間に発生
する磁界の分布を均一化したことを特徴とするものであ
る。
The present invention provides a cylindrical conductor around the electrode, and! The feature is that the distribution of the magnetic field generated between the poles is made uniform.

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

以下本発明の一実施例を図面(=よって説明する。 An embodiment of the present invention will be described below with reference to the drawings.

弗1図は本発明の真空バルブの一実施例を示す。Figure 1 shows an embodiment of the vacuum valve of the present invention.

従来の縦磁界方式の真空バルブと異なる点は第3図のシ
ールド9を円筒導体11(=置き替えている点である。
The difference from the conventional vertical magnetic field type vacuum valve is that the shield 9 in FIG. 3 is replaced with a cylindrical conductor 11 (==).

円筒導体IN=は導電率のよい銅やアルミニウム等の材
料が使用される。
For the cylindrical conductor IN=, a material having good conductivity such as copper or aluminum is used.

周知のよう(=導電率の高い材料においては、交流電磁
界が導体の表面Jffl i二局限されて内部に人らな
い現象、すなわち表皮効果が顕著となる。電磁界が表面
強度の1/e (=なる厚さδは、δ=(2/μσω)
2で与えられる。ここでμは透磁率、σは導電率、ωは
電磁界の角周波数である。例えばCu材料の場合、50
Hzの縦磁界に対するδは93.5朋(=なる。実際に
は、アークプラズマの変動礁二対する導体壁の安全化効
果があるため導体の厚さを上1己δの30%以上とする
ことによ電磁界の脹みを抑制し又縦磁界中のアークプラ
ズマを安定化できるので、しゃ断性能が向上する。ただ
し高導電率材料の円周方向(−1個所以上、軸方向に溝
を設け、この溝の部分には何も入れない場合や高抵抗体
を入れて、縦磁界に直角な平面内で円周方向へのターン
Kttiが導体内をaれることを防止し、縦磁界が打消
されることを防ぐ必要がある。円筒導体11の内径が、
主電極6a、7a外径4;近い程、磁界均一化の効果は
大きくなる。
As is well known (= in materials with high conductivity, the alternating current electromagnetic field is localized to the surface of the conductor and there is no one inside, that is, the skin effect becomes noticeable.The electromagnetic field is 1/e of the surface intensity. (=Thickness δ is δ=(2/μσω)
It is given by 2. Here, μ is magnetic permeability, σ is electrical conductivity, and ω is the angular frequency of the electromagnetic field. For example, in the case of Cu material, 50
δ for a vertical magnetic field of Hz is 93.5 mm (==.Actually, the thickness of the conductor is set to 30% or more of δ in order to have a safety effect on the conductor wall against the fluctuation of the arc plasma. In particular, the expansion of the electromagnetic field can be suppressed and the arc plasma in the vertical magnetic field can be stabilized, so the breaking performance is improved. If nothing is inserted into this groove, or a high-resistance material is inserted, the circumferential turn Ktti in the plane perpendicular to the longitudinal magnetic field is prevented from being averted inside the conductor, and the longitudinal magnetic field is It is necessary to prevent this from being canceled out.The inner diameter of the cylindrical conductor 11 is
Main electrodes 6a, 7a outer diameter 4: The closer they are, the greater the effect of uniformizing the magnetic field.

以上述べた理由によシ土電極間の縦磁界分布は第1図の
縦磁界1(H二示すよう(=均一とな9又縦磁界中のア
ークプラズマを安定化できるのでアークプラズマからの
粒子損失が減少し、アーク電圧が低く抑えられるため電
mL遮断性能が向上するほか電極への注入エネルギーが
低下し電極消耗量が減少する。また、従来の真空バルブ
のようにシールドと磁力線が交わることがなくなるため
アークプラズマ(=よる導体の損傷は小さい。
For the reasons stated above, the vertical magnetic field distribution between the earth electrodes is uniform as shown in Figure 1 (Figure 1). Loss is reduced and arc voltage is suppressed to a low level, which improves electric mL interrupting performance and reduces the energy injected into the electrode, reducing electrode wear.In addition, the shield and magnetic field lines do not intersect as in conventional vacuum valves. The damage to the conductor caused by the arc plasma is small.

円筒導体11が縦磁界を打消すことのないように、円筒
導体11の一部に纒を設け、溝(=は何も入れない場合
や胃抵抗体(絶縁物でも良い)を入れる必要のあること
は先ζ;述べたが高抵抗体として、例えばステンレスベ
ローズを円周方間に便用することでも良い。このように
すると溝を入れた場合と比較して円筒等体が一体化する
という利点があシ、4抵抗体として絶縁物を入れた場合
と比較して、アークプラズマが衝突した際(=、多量の
ガスが発生しないという利点がある。
In order to prevent the cylindrical conductor 11 from canceling the vertical magnetic field, a part of the cylindrical conductor 11 is provided with a thread, and a groove (= means that nothing is inserted or a gas resistor (an insulator may be used) must be inserted. As mentioned earlier, it is also possible to use stainless steel bellows, for example, in the circumferential direction as a high-resistance material.In this way, the cylindrical body is integrated compared to the case where grooves are provided. Compared to the case where an insulator is used as the four resistors, there is an advantage that a large amount of gas is not generated when the arc plasma collides.

また円筒導体に溝を入れるのではなく円筒導体を複数個
に分割して各々を支持する構成もある。
There is also a configuration in which the cylindrical conductor is divided into a plurality of parts and each part is supported instead of forming a groove in the cylindrical conductor.

さらに第1図では導体を真空容器内に配置しているが、
これを絶縁容器1の外部(=配置しても良いことは言う
゛までもない。
Furthermore, in Figure 1, the conductor is placed inside a vacuum container, but
It goes without saying that this may be placed outside the insulating container 1.

第2図に示す例は、円筒導体11を真空容器の一部とし
て使用したものであり、この場合は円筒導体11の溝に
は高抵抗体を円周方図に人れる密封構造(ニする必要が
ある。このようにすると真空バルブの外径を小さくする
ことができる。
In the example shown in Fig. 2, the cylindrical conductor 11 is used as part of a vacuum vessel. Yes, this allows the outer diameter of the vacuum valve to be reduced.

円筒導体11による磁界均一化の効果は主電極外周と円
筒導体間距離力;小さい程大きいが、この場合主電極間
に発生したアークプラズマ粒子の拡散等によ9円14体
を介して土&[間(=アーク′題流が流れる恐れがある
。円筒導体には電極材料とは異なる材料の使用が一般的
であるため電流遮断能力の低下がおこる場合も生ずる。
The effect of uniformizing the magnetic field by the cylindrical conductor 11 is the distance force between the main electrode outer periphery and the cylindrical conductor; There is a risk that an arc current may flow. Since the cylindrical conductor is generally made of a material different from the electrode material, the current interrupting ability may be reduced.

そこで円筒導体内面に絶縁物を設けることによシ円筒導
体を介して電流が流れる事を防ぐ一方、円筒導体を生電
極−二近づけて、磁界均一化の効果を大きく作用させる
ことができる。
Therefore, by providing an insulator on the inner surface of the cylindrical conductor, it is possible to prevent current from flowing through the cylindrical conductor, and at the same time, by bringing the cylindrical conductor closer to the live electrode, the effect of uniformizing the magnetic field can be greatly increased.

〔発明の効果〕〔Effect of the invention〕

本発明(=よれば、電極の周囲に円筒導体を設けること
によυ大屯υtf;越断能力(=優れた高信頼性で長寿
命の真空バルブを提供することができる。
According to the present invention, by providing a cylindrical conductor around an electrode, it is possible to provide a vacuum valve with excellent reliability and long life.

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

第1図は本発明による真空ノ(ルプの一実施例を示す縦
断面図、第2図は本発明(=よる真空ノ(ルフ。 の他の実施例を示す縦断面図、第3図は従来の真空バル
ブの縦断面図、第4図は主題極間に発生する縦磁界の分
布を示す説明図である。 11・・・円筒導体 (7317)  代理人 弁理士 則 近 jl!  
佑(#デカ)1名)第1図 第2図 第3図 第4図
FIG. 1 is a vertical sectional view showing one embodiment of the vacuum nozzle according to the present invention, FIG. 2 is a longitudinal sectional view showing another embodiment of the vacuum nozzle according to the present invention, and FIG. Fig. 4, a vertical cross-sectional view of a conventional vacuum valve, is an explanatory diagram showing the distribution of the vertical magnetic field generated between the subject poles. 11...Cylindrical conductor (7317) Agent Patent attorney Rule Chika jl!
Yu (#deka) 1 person) Figure 1 Figure 2 Figure 3 Figure 4

Claims (1)

【特許請求の範囲】[Claims] 真空容器とこの真空容器内に開閉自在に配置された一対
の電極と電流遮断時に前記電極間に発生するアークに対
し、それと平行な磁界を発生させる前記電極の裏面に配
置したコイル電極を有する真空バルブにおいて、前記電
極の周囲に配置した円筒導体を前記真空容器に取付け、
この円筒導体は軸方向に1個以上の溝を有し、この溝が
高抵抗体で構成されていることを特徴とする真空バルブ
A vacuum comprising a vacuum container, a pair of electrodes arranged in the vacuum container so as to be openable and closable, and a coil electrode arranged on the back side of the electrodes to generate a magnetic field parallel to the arc generated between the electrodes when current is interrupted. In the valve, a cylindrical conductor arranged around the electrode is attached to the vacuum container,
A vacuum valve characterized in that the cylindrical conductor has one or more grooves in the axial direction, and the grooves are made of a high-resistance material.
JP14220184A 1984-07-11 1984-07-11 Vacuum bulb Pending JPS6122524A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14220184A JPS6122524A (en) 1984-07-11 1984-07-11 Vacuum bulb

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14220184A JPS6122524A (en) 1984-07-11 1984-07-11 Vacuum bulb

Publications (1)

Publication Number Publication Date
JPS6122524A true JPS6122524A (en) 1986-01-31

Family

ID=15309739

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14220184A Pending JPS6122524A (en) 1984-07-11 1984-07-11 Vacuum bulb

Country Status (1)

Country Link
JP (1) JPS6122524A (en)

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