JPS61292830A - Vacuum interruptor - Google Patents
Vacuum interruptorInfo
- Publication number
- JPS61292830A JPS61292830A JP60134814A JP13481485A JPS61292830A JP S61292830 A JPS61292830 A JP S61292830A JP 60134814 A JP60134814 A JP 60134814A JP 13481485 A JP13481485 A JP 13481485A JP S61292830 A JPS61292830 A JP S61292830A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- movable
- fixed
- fixed electrode
- 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
Links
- 239000002184 metal Substances 0.000 claims description 52
- 229910052751 metal Inorganic materials 0.000 claims description 52
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 claims description 27
- 238000013459 approach Methods 0.000 claims description 3
- 239000000463 material Substances 0.000 description 12
- 230000000694 effects Effects 0.000 description 10
- 230000005684 electric field Effects 0.000 description 9
- 238000004663 powder metallurgy Methods 0.000 description 7
- 230000002093 peripheral effect Effects 0.000 description 6
- 239000002245 particle Substances 0.000 description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 239000002131 composite material Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000017525 heat dissipation Effects 0.000 description 4
- 230000005426 magnetic field effect Effects 0.000 description 4
- 239000000203 mixture Substances 0.000 description 4
- 239000003870 refractory metal Substances 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 239000007772 electrode material Substances 0.000 description 3
- 230000000903 blocking effect Effects 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 230000000116 mitigating effect Effects 0.000 description 2
- 238000010008 shearing Methods 0.000 description 2
- 229910000531 Co alloy Inorganic materials 0.000 description 1
- NMFHJNAPXOMSRX-PUPDPRJKSA-N [(1r)-3-(3,4-dimethoxyphenyl)-1-[3-(2-morpholin-4-ylethoxy)phenyl]propyl] (2s)-1-[(2s)-2-(3,4,5-trimethoxyphenyl)butanoyl]piperidine-2-carboxylate Chemical compound C([C@@H](OC(=O)[C@@H]1CCCCN1C(=O)[C@@H](CC)C=1C=C(OC)C(OC)=C(OC)C=1)C=1C=C(OCCN2CCOCC2)C=CC=1)CC1=CC=C(OC)C(OC)=C1 NMFHJNAPXOMSRX-PUPDPRJKSA-N 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 229910000963 austenitic stainless steel Inorganic materials 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000003628 erosive effect Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
- 230000005012 migration Effects 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 239000010902 straw Substances 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Landscapes
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
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】
A、産業上の利用分野
本発明は、しゃ断能力を向上させた縦磁界印加式の真空
インタ2ブタに関する。DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a vertical magnetic field application type vacuum interrupter with improved breaking ability.
B0発明の概要
この発明は、固定電極側の金属端板の外側にコイルを具
えた縦磁界印加式の真空インタラプタにおいて。B0 Summary of the Invention The present invention relates to a vertical magnetic field application type vacuum interrupter that includes a coil on the outside of a metal end plate on the fixed electrode side.
可動電極の外径寸法を固定電極の外径寸法よシも大きく
するとともに可動電極の背後に緩和シールドを具え、金
属端板と固定電極との隙間を一定の範囲内に設定するこ
とにより。By making the outer diameter of the movable electrode larger than that of the fixed electrode, providing a relaxation shield behind the movable electrode, and setting the gap between the metal end plate and the fixed electrode within a certain range.
極性効果、電界集中を防止するだけでなく固定電極から
金属端板へのアークの移行を防止してしゃ断能力を向上
させたものである。This not only prevents polarity effects and electric field concentration, but also prevents arc migration from the fixed electrode to the metal end plate, improving breaking ability.
C1従来の技術
真空インタラプタには、しゃ断能力([流しゃ断性能、
耐電圧性能)1向上させるために両電極間に生じるアー
クと平行に磁界を印加する縦磁界印加式の真空インタラ
プタがある。C1 Conventional technology Vacuum interrupters have a breaking capacity (flow breaking performance,
In order to improve withstand voltage performance) 1, there is a vertical magnetic field application type vacuum interrupter that applies a magnetic field parallel to the arc generated between both electrodes.
縦磁界印加式の真空インタラプタには、真空容器の外周
にコイルを具えたものと、真空容器の内部であって少な
くとも一方の電極の背後にコイルを具えたものとがある
。前者はコイルからの放熱性が良いが真空容器の外周に
コイルを具えることから外径が大きくなって大形化する
という欠点がある。−万、後者は真空容器内にコイルが
収まるため小形化できるが1発熱源となるコイルは真空
容器内にあるため放熱性が悪く、しかも開閉の衝繋がコ
イルに作用し耐久性が悪いという欠点がある。There are two types of vertical magnetic field application type vacuum interrupters: those equipped with a coil around the outer periphery of a vacuum container, and those equipped with a coil inside the vacuum container behind at least one electrode. The former has good heat dissipation from the coil, but has the disadvantage that the outer diameter becomes large because the coil is provided around the outer periphery of the vacuum container. -The latter can be made smaller because the coil is housed inside the vacuum container, but the disadvantage is that the heat dissipation is poor because the coil, which is the source of heat generation, is inside the vacuum container, and the durability is poor because the contact between opening and closing acts on the coil. There is.
そのため、−万の電極の背後であってかつ真空容器の外
部(金属端板の外@)にコイルを具えた縦磁界印加式の
真空インタラプタが提案されている。斯かる真空インタ
ラプタの断面図を第6図に示す。図のようにアルミナセ
ラミックス等からなる絶縁筒1aとオーステナイト系ス
テンレス鋼(以下susと略すンの5us104 Lか
らなる金属筒1bと金属端板2,8等から真空容器4が
1R放されてお夕、真空容器4の内部に相互に接近、離
反可能な固定リード棒6と可動リード棒7とが導入され
ている。固定リード棒6.可動リード棒7の内端部には
Cu −Mo −Cr(例えばCu −25Mo −7
Cr )の組成からなりかつ粉末冶金法による複合材料
からなる固定電極8.可動電極9が固着されてお九固定
電極8の背後であって真空容器4の外部にはコイル[0
が具えられている。このCu Mo−Crに代表され
るCu−耐火金属−鉄族元素の組成からなりかつ粉末冶
金法による複合材料は、しゃ断能力の優れていることは
特開昭59−27418.特開昭59−119825.
特開昭59−11%26、特開昭60−1821.特開
昭60−3822等で知られている。なお、 11はシ
ールドであって固定電極8と同電位である。12はベロ
ーズ。Therefore, a vertical magnetic field application type vacuum interrupter has been proposed that includes a coil behind the -10,000 electrode and outside the vacuum container (outside the metal end plate). A cross-sectional view of such a vacuum interrupter is shown in FIG. As shown in the figure, the vacuum vessel 4 is released 1R from the insulating tube 1a made of alumina ceramics, etc., the metal tube 1b made of 5us104 L of austenitic stainless steel (hereinafter abbreviated as SUS), and the metal end plates 2, 8, etc. A fixed lead rod 6 and a movable lead rod 7 that can approach and separate from each other are introduced into the vacuum chamber 4.The inner ends of the fixed lead rod 6 and the movable lead rod 7 are coated with Cu-Mo-Cr. (For example, Cu-25Mo-7
8. Fixed electrode made of a composite material made of a powder metallurgy method and having a composition of Cr). A movable electrode 9 is fixed, and a coil [0
is provided. It has been reported in JP-A No. 59-27418 that a composite material composed of Cu-refractory metal-iron group element represented by Cu Mo-Cr and produced by powder metallurgy has excellent breaking ability. Japanese Patent Publication No. 59-119825.
JP-A-59-11%26, JP-A-60-1821. It is known from Japanese Patent Application Laid-Open No. 60-3822. Note that 11 is a shield and has the same potential as the fixed electrode 8. 12 is bellows.
13ハペローズシールドである。また、固定電極8と金
属端板2とを接触させているのは、固定電極8と可動電
極9との間における縦磁界効果を十分なものにするため
にはコイル10と一対の電極空間とをできるだけ接近さ
せた方がよいからである。13 Haperose Shield. Furthermore, the fixed electrode 8 and the metal end plate 2 are brought into contact with each other in order to ensure a sufficient longitudinal magnetic field effect between the fixed electrode 8 and the movable electrode 9. This is because it is better to have them as close as possible.
前記真空インタラプタによれば、真空容器の外にコイル
が具えられているので放熱性が曳く、シかも開閉時の衝
藁が直接コイルに作用しないので耐久性もよい。また、
コイルは真空容器の外周部には具えられていないので径
方向の小形化が図れる。つま)、小形化、放熱性、耐久
性等の点において優れている。According to the vacuum interrupter, since the coil is provided outside the vacuum container, heat dissipation is improved, and the durability is also good because the straw during opening and closing does not directly act on the coil. Also,
Since the coil is not provided on the outer periphery of the vacuum container, the size can be reduced in the radial direction. It is excellent in terms of size, heat dissipation, durability, etc.
しかし、可動電極9の近傍では可動電極9がコイル【0
から離れているために磁力線14が外側へわん曲し、し
ゃ断性能に極性効果が生じる。即ち。However, in the vicinity of the movable electrode 9, the movable electrode 9 has a coil of
Since the magnetic field lines 14 are far away from each other, the lines of magnetic force 14 are curved outward, causing a polar effect on the breaking performance. That is.
交流電流しゃ断時において固定電極8がプラス電位にあ
る場合に比べ、マイナス電位にある場合はしゃ断性能が
劣ることになる。この理由は、コイル10によって発生
する磁力線14が固定電極8から可動電極9へ同かうに
つれて外側へわん曲してhることによる。つまp、しゃ
断時において荷電粒子が可動電極9から発生している場
合には荷電粒子は磁力酬に沿って固定電極に効果的に捕
捉されるが、荷電粒子が固定電極8から発生する場合に
は一部(周辺部]の荷電粒子は磁力線に沿って可動電極
9に捕捉されることなく真空容器内に拡散するからであ
る。When the fixed electrode 8 is at a negative potential, the breaking performance is inferior to that when the fixed electrode 8 is at a positive potential when cutting off an alternating current. The reason for this is that the magnetic lines of force 14 generated by the coil 10 curve outward as they move from the fixed electrode 8 to the movable electrode 9. When the charged particles are generated from the movable electrode 9 at the time of shutoff, the charged particles are effectively captured by the fixed electrode along the magnetic flux, but when the charged particles are generated from the fixed electrode 8, This is because some (peripheral) charged particles diffuse into the vacuum container along the lines of magnetic force without being captured by the movable electrode 9.
そこで、可動電極の外径寸法を固定電極の外径寸法より
も大きく設定してしゃ断性能を調べてみたところ次のよ
うな結果が得られた。固定電極と可動電極との外径寸法
を同一にした場合において。Therefore, when we set the outer diameter of the movable electrode to be larger than the outer diameter of the fixed electrode and investigated the breaking performance, we obtained the following results. When the outer diameter dimensions of the fixed electrode and the movable electrode are the same.
固定電極側にプラスの電流を印加した場合のしゃ断性能
t−100とした場合、マイナスの電流を印加した場合
のしゃ断性能は80であった。一方、可動電極の外径寸
法t−10%大きくシ九ときのしゃ断性能は夫々110
、90であった。これh可動電極の外径音大きくする
ことにより、磁力線がわん曲しているにもかかわらず、
固定電極から発生する荷電粒子が可動電極に捕捉されて
極性効果がなくなることを示している。When the breaking performance was t-100 when a positive current was applied to the fixed electrode side, the breaking performance was 80 when a negative current was applied. On the other hand, when the outer diameter of the movable electrode is increased by t-10%, the breaking performance is 110, respectively.
, 90. By increasing the outer diameter of the movable electrode, even though the lines of magnetic force are curved,
This shows that charged particles generated from the fixed electrode are captured by the movable electrode, eliminating the polarity effect.
ところが、可動電極の外径を大きくした場合。However, when the outer diameter of the movable electrode is increased.
断念な問題が生じた。即ち、第7図のように固定電極8
と同電位のシールド11との間において、可動電極9の
外径寸法が大きくなった分だけ可動電極9の外周部にお
ける電界集中が著しくなる。図中、15は等電位線であ
シ、可動電極9の外周部に電界が集中していることがわ
かる。そのため耐電圧性能が低くなり、シゃ断M後の過
渡回復電圧に耐えられず、結果的にはし中断性能が同上
しないという問題がある。An irresistible problem arose. That is, as shown in FIG.
As the outer diameter of the movable electrode 9 increases, the electric field concentration at the outer periphery of the movable electrode 9 becomes significant between the movable electrode 9 and the shield 11 having the same potential. In the figure, reference numeral 15 indicates equipotential lines, and it can be seen that the electric field is concentrated on the outer periphery of the movable electrode 9. Therefore, there is a problem in that the withstand voltage performance is lowered and cannot withstand the transient recovery voltage after the interruption M, and as a result, the interruption performance is not the same.
この傾向は、第7図のように金属端板2及び金属筒1b
ft介して固定電極8と同電位になつ九金属部材として
のシールド11で一対の電極9t−囲っている場合の方
が、所謂中間電位の中間シールドで一対の電極を囲って
いる場合よシも、電位差が大きくなるぶんだけ電界強度
が大きくなって著しいものとなる。This tendency is reflected in the metal end plate 2 and the metal tube 1b as shown in FIG.
It is better to surround the pair of electrodes 9t with a shield 11 which is a metal member that has the same potential as the fixed electrode 8 through ft than to surround the pair of electrodes with a so-called intermediate shield having an intermediate potential. As the potential difference increases, the electric field strength increases and becomes significant.
斯かる問題を解決する九め、第8図に示すようにコイル
t−有しない可動電極の外径寸法金コイルを有する固定
電極の外径寸法よシ大きくするとともに、コイルを有し
ない可動電極の外周部近傍での電界集中を防止する光め
、可動リード棒の内端部を囲繞するとともに可動電極の
外周面から可動リード棒の外周面まで延びる緩和シール
ドを具えた真空インタラプタを考案した。The ninth step to solving this problem is to make the outer diameter of the movable electrode without a coil larger than that of the fixed electrode with a gold coil, as shown in Figure 8, and to increase the outer diameter of the movable electrode without a coil. We have devised a vacuum interrupter that includes a light to prevent electric field concentration near the outer periphery, and a relaxation shield that surrounds the inner end of the movable lead rod and extends from the outer periphery of the movable electrode to the outer periphery of the movable lead rod.
第8図において、可動電極9の外径寸法は前記のように
固定電極8の外径寸法よりも10%位大きく設定されて
お夕、可動電極9の背後に緩和シールド16が具えられ
ている。背後とは、可動リード棒7が固着されている側
をいい、第8図中、可動電極9の真下をいう。緩和シー
ルド16は可動リード棒7の内端部を囲繞して可動電極
9の外周面近傍から可動リード棒7の外周面までゆるや
かにのばして設けられている。つまり、緩和シールド1
6はラッパ状に形成され、小径部に穿設された孔16b
へ可動リード棒7が挿通して固着され、大径部の端は可
動電極9の外周面近傍で内側へ大きく曲げてカール部1
6&が形成されている。In FIG. 8, the outer diameter of the movable electrode 9 is set approximately 10% larger than the outer diameter of the fixed electrode 8 as described above, and the relaxation shield 16 is provided behind the movable electrode 9. . The back side refers to the side to which the movable lead rod 7 is fixed, and refers to the side directly below the movable electrode 9 in FIG. The relaxation shield 16 is provided to surround the inner end of the movable lead rod 7 and to extend gently from the vicinity of the outer peripheral surface of the movable electrode 9 to the outer peripheral surface of the movable lead rod 7. In other words, mitigation shield 1
6 is a hole 16b formed in a trumpet shape and bored in the small diameter part.
The movable lead rod 7 is inserted into and fixed to the movable lead rod 7, and the end of the large diameter portion is bent greatly inward near the outer peripheral surface of the movable electrode 9 to form a curled portion 1.
6& is formed.
緩和シールド16は電界集中を防止するために設けられ
るので、可動電極9の外周面から可動リード棒7の外周
面までゆるやかな曲面に形成されている。ま九、緩和シ
ールド16の最大外径寸法は可動電極9の外径寸法と略
同じ大きさとなっている。Since the relaxation shield 16 is provided to prevent electric field concentration, it is formed into a gently curved surface from the outer circumferential surface of the movable electrode 9 to the outer circumferential surface of the movable lead rod 7. (9) The maximum outer diameter of the relaxation shield 16 is approximately the same as the outer diameter of the movable electrode 9.
これは、可動電極9の外径寸法よシも大きくすると緩和
シールド16ヘアークが移行してしゃ断性能が低下し、
逆に可動電極9の外径寸法よシも小さくすると緩和シー
ルド16t−設けない場合と同様の理由で可動電極9の
外層面近傍に電界が集中してやはりしゃ断性能が低下す
るからである。緩和シールドとしてはこのほか#!9図
(a) # (b)に示す形状のもので4よい。This is because when the outer diameter of the movable electrode 9 is increased, the hair arc of the relaxation shield 16 shifts and the breaking performance decreases.
On the other hand, if the outer diameter of the movable electrode 9 is made smaller, the electric field will concentrate near the outer surface of the movable electrode 9 for the same reason as when the relaxation shield 16t is not provided, resulting in a decrease in the breaking performance. In addition to this as a mitigation shield #! The shape shown in Figure 9 (a) # (b) is enough.
D9発明が解決しようとする問題点
ところが、しゃ断能力は、予定していたほどけ向上しな
かっな。そこで分解して調べてみたところ。Problems that the D9 invention aims to solve However, the breaking ability did not improve as much as expected. So I took it apart and looked into it.
固定電極周辺の金属端板にアークが移行してエロージョ
ンの痕跡が見つかつ九。このことから、可動電極を大き
くして極性効果をなくそうとしたものの、アークが固定
電極から金Is端板へ移行してしまい、可動電極から発
生したベーパーが磁力線によって安定して捕捉されると
は限らないということがわかつ九。Traces of erosion due to arc transfer to the metal end plate around the fixed electrode were found. Based on this, although we tried to eliminate the polarity effect by making the movable electrode larger, the arc migrated from the fixed electrode to the gold Is end plate, and the vapor generated from the movable electrode was stably captured by the magnetic lines of force. It turns out that there are no limitations.
斯かる事実から、固定電極と金属端板との隙間がしゃ断
能力に影響を与えるのではないかと推察し比。Based on this fact, we inferred that the gap between the fixed electrode and the metal end plate affected the breaking ability.
本発明は1以上の点に鑑みてなされ九ものであシ、固定
電極と金属端板との隙間を所定の範囲にすることによっ
て、しゃ断能力が最も高い縦磁界印加式の真空インタラ
プタを提供することを目的とする。The present invention has been made in view of one or more points, and provides a vertical magnetic field application type vacuum interrupter with the highest interrupting ability by setting the gap between the fixed electrode and the metal end plate within a predetermined range. The purpose is to
E1問題点を解決する九めの手段 斯かる目的全達成するための本発明の構成社。Ninth way to solve E1 problem The composition of the present invention is to achieve all of these objectives.
絶縁筒の両端に金属端板を固着して形成された真空容器
の内部に前記金属端板を貫通して相互に接近・離反可能
に固定リード棒及び可動リード棒を導入するとともに固
定リード棒、可動リード棒のVg端部に夫々固定電極、
可動電極を固着しかつ固定電極側の金属端板の外側に縦
磁界発生コイルを具え九真空インクラブタにおいて、可
動電極の外径寸法を固定電極の外径寸法より°大きく形
成するとともに両電極を固定電極と同電位の金属部材で
囲繞し、可動リード棒の内端部を囲繞して可動リード棒
の外周面から可動電極の外周面までのびる緩和シールド
を具え、前記固定電極と固定側の前記金属端板との隙間
を2mm以上で前記固定電極の外径寸法の30%以下に
設定したことt−%徴とする。A fixed lead rod and a movable lead rod are introduced into a vacuum container formed by fixing metal end plates to both ends of an insulating cylinder so as to penetrate through the metal end plates so as to be able to approach and separate from each other, and a fixed lead rod; A fixed electrode is attached to each Vg end of the movable lead rod.
In a nine-vacuum incrector in which the movable electrode is fixed and a vertical magnetic field generating coil is provided on the outside of the metal end plate on the fixed electrode side, the outer diameter of the movable electrode is formed to be larger than the outer diameter of the fixed electrode, and both electrodes are fixed. A relaxation shield is provided, which is surrounded by a metal member having the same potential as the electrode, surrounds the inner end of the movable lead rod, and extends from the outer peripheral surface of the movable lead rod to the outer peripheral surface of the movable electrode, and the fixed electrode and the metal on the fixed side are provided. It is assumed that the gap with the end plate is set to 2 mm or more and 30% or less of the outer diameter of the fixed electrode.
20作用
可動電極の外径寸法を固定電極の外径寸法よ)も大きく
することによって極性効果をなくシ、可動電極を大きく
することによって生じる電界集中を緩和シールドによっ
て緩和し、固定電極から金属端板ヘアークが移動してし
中1!?能力が低下するのを防止するために固定電極と
金属端板との隙間を2u以上でかつ固定電極外径寸法の
30 %以下に設定しているので、し中断能力の高い真
空インタラプタが提供できる。20 By increasing the outer diameter of the working movable electrode (as compared to the outer diameter of the fixed electrode), the polarity effect is eliminated, and the electric field concentration caused by increasing the size of the movable electrode is alleviated by the relaxation shield, and the The board hair arc has moved and it's 1st year in middle school! ? In order to prevent the capacity from decreasing, the gap between the fixed electrode and the metal end plate is set to 2u or more and 30% or less of the fixed electrode outer diameter, so we can provide a vacuum interrupter with high interrupting capacity. .
G、実施例
以下1本発明を図面に示す実施例に基づいて詳細に説明
する。G. Embodiments The present invention will be explained in detail below based on embodiments shown in the drawings.
まず、電極及び金属端板上形成する材料のしゃ断能力を
、第8図に示す構造の真空インタラプタを用いて実験し
た。図中、17は一対の絶縁筒28と金属端板26 、
27とからなる真空容器、18は固定リード棒、19は
可動リード棒、20は固定電極、21は可動電極、22
はベローズ、23は中間シールド、24はベローズシー
ルド、25は固定リード棒18に対して直列に接続され
た縦磁界発生コイルである。First, the breaking ability of the material formed on the electrode and the metal end plate was tested using a vacuum interrupter having the structure shown in FIG. In the figure, 17 is a pair of insulating cylinders 28 and metal end plates 26,
27 is a vacuum container, 18 is a fixed lead rod, 19 is a movable lead rod, 20 is a fixed electrode, 21 is a movable electrode, 22
23 is a bellows, 23 is an intermediate shield, 24 is a bellows shield, and 25 is a vertical magnetic field generating coil connected in series to the fixed lead rod 18.
第4図は、第8図に示す真空インタラプタで実験し念結
果を示すもので、材料の異なる電極を用いた場合の電極
径としゃ断電流との関係を示すグラフである。図中、(
イ)はCu −25Mo −7Crの組成である粉末冶
金法による複合材料、(ロ)は8U8804L。FIG. 4 shows the experimental results using the vacuum interrupter shown in FIG. 8, and is a graph showing the relationship between the electrode diameter and the cutoff current when electrodes made of different materials are used. In the figure, (
A) is a composite material made by powder metallurgy with a composition of Cu-25Mo-7Cr, and (B) is 8U8804L.
(/号はF・及びFe −N1− Co合金、(−1は
Cu t″各々電極材料とした場合を示している。この
実験における印加電圧は12KV(r、m、s )であ
シ1両電極間のギャップは12mである。なお、(ロ)
、←→、に)の材料は金属端板上形成する材料として広
く用いられている。(/ indicates F and Fe-N1-Co alloys, (-1 indicates the case where Cu t'' is used as the electrode material.The applied voltage in this experiment was 12 KV (r, m, s). The gap between both electrodes is 12 m.
, ←→, ni) are widely used as materials for forming metal end plates.
第5図に示すのは、同様に材料の異なる電極音用いた場
合の電極間ギャップと耐電圧との関係を示すグラフであ
フ1図中、ケ)〜に)は第4図で示したものと同一の材
料を電極とした場合を示している。なお、電極外径は5
0mで電極厚さは6nであって、グラフは25KAの電
流を10回しゃ断した後の ′耐電圧特性を示している
。Figure 5 is a graph showing the relationship between the interelectrode gap and withstand voltage when electrodes made of different materials are used. This shows the case where the electrodes are made of the same material. In addition, the electrode outer diameter is 5
The electrode thickness is 6n at 0 m, and the graph shows the withstand voltage characteristics after a current of 25 KA was cut off 10 times.
第4図及び第5図の結果から、粉末冶金法によるCu
−Mo −Crは5US−?Cu等よ〕も電流しゃ断性
能、耐電圧性能のいずれ本が良好なことがわかった。特
にSUSは一般には耐電圧性能が良好な材料として知ら
れているが、アークを引いた場合には耐電圧性能があま
り良くないことがわかつ九。From the results shown in Figures 4 and 5, it is clear that Cu by powder metallurgy
-Mo -Cr is 5US-? Cu, etc.] was also found to have good current cutoff performance and withstand voltage performance. In particular, SUS is generally known as a material with good withstand voltage performance, but when an arc is drawn, it is found that the withstand voltage performance is not very good9.
これらのことから第8図の真空インタラプタを検討する
と、電極はCu −Mo −Crであり金属端板は5U
S804L であることから固定電極の背後にこの電極
を構゛成する材料(Cu −Mo −Cr )よシもし
ゃ断能力(電流しゃ断性能、耐電圧性能)の点で劣るS
O8部材が存在していることになる。Considering the vacuum interrupter shown in Fig. 8 based on these facts, the electrodes are Cu-Mo-Cr and the metal end plate is 5U.
Because it is S804L, there is a S804L material behind the fixed electrode that is inferior to the material (Cu-Mo-Cr) that makes up this electrode in terms of blocking ability (current blocking performance, withstand voltage performance).
This means that the O8 member is present.
そして、固定電極の直背後にこれよシ材質的にしゃ断能
力の劣る金属端板が広い面積で存在している九め、アー
クの足が固定電極から外れて金属端板へ移行した場合に
あっては、電流しゃ断性能及び耐電圧性能に対して金属
端板の特性が顕著に悪影響を及ぼすことがわかった。Furthermore, there is a large area of metal end plate directly behind the fixed electrode, which is inferior in breaking ability due to its material. It was found that the characteristics of the metal end plate had a significant negative effect on the current interrupting performance and withstand voltage performance.
そこで、固定電極を金属端板からどれくらい離せばアー
クが電極から金属端板へ移行しないかを調べると共に、
どれくらい離すと縦磁界効果が減少するかを調べた。Therefore, we investigated how far away the fixed electrode should be from the metal end plate to prevent the arc from transferring from the electrode to the metal end plate.
We investigated how far away the longitudinal magnetic field effect can be reduced.
即ち、第1図に示す真空インタラプタを用いて固定電極
と金属端板との隙間を変化させてしゃ断性能を調べた。That is, using the vacuum interrupter shown in FIG. 1, the interruption performance was investigated by varying the gap between the fixed electrode and the metal end plate.
実験に用いた真空インタラプタの各部の寸法は、第1図
において、金属筒の外径a= 110 xx 、コイル
の外径b−100絽、コイルの内径e = 80m 、
固定リード棒の外径d = 30龍、コイルの高さ・=
15m、コイル下面と金属端板の上面との間の寸法f−
2m 、金属端板の厚さg z 8 t*。The dimensions of each part of the vacuum interrupter used in the experiment are as shown in Fig. 1: outer diameter of the metal tube a = 110 xx, outer diameter of the coil b - 100 mm, inner diameter of the coil e = 80 m,
Fixed lead rod outer diameter d = 30mm, coil height =
15m, dimension f- between the bottom surface of the coil and the top surface of the metal end plate
2 m, thickness of metal end plate g z 8 t*.
電極の厚さり、5絽であり、コイルIOKよって発生す
る磁界が固定電極8及び可動電極9の全面に作用するよ
うに、C≧D(固定電極の外径)となっている。なお、
29は絶縁物である。斯かる真空インタラゲタにおいて
、固定電極8と金属端板2との隙間tを変化させ几場合
のしゃ断電流の相対値全第2図に示す、この相対値は、
粉末冶金法によるCu −25Mo −7Cr から
なる電極を用いるとともにSUS 804 L からな
る金属端板を用いて縦磁界を印加し九ときのしゃ断限界
電流の大きさを基準の100%として示したものである
0図中、(ホ)はD=60(絽)としてSUS 304
L端板金層いた場合、(へ)はD−50(關]として
8U8804 L端板上用いた場合を示しており、各場
合における電極は粉末冶金によるCu −25Mo −
7Crである。なお、可動電極外径は、各々u X D
(a+)である。The thickness of the electrode is 5 电, and C≧D (outer diameter of the fixed electrode) so that the magnetic field generated by the coil IOK acts on the entire surface of the fixed electrode 8 and the movable electrode 9. In addition,
29 is an insulator. In such a vacuum interrogator, the relative values of the cut-off current when the gap t between the fixed electrode 8 and the metal end plate 2 is changed are as shown in FIG.
An electrode made of Cu-25Mo-7Cr made by powder metallurgy was used, and a vertical magnetic field was applied using a metal end plate made of SUS 804L. In a certain diagram, (E) is SUS 304 with D=60 (紽)
When there is an L end sheet metal layer, (f) shows the case where it is used as D-50 on the 8U8804 L end plate, and the electrode in each case is Cu-25Mo- made by powder metallurgy.
It is 7Cr. In addition, the outer diameter of the movable electrode is
(a+).
図中* p、 a Ptはtの値が小さいためにアーク
が電極8から金属端板2へ移行して電流し千断性能が低
くなっている範囲を示してお5−Qx−Qtは電流しや
断性能ft100 ’16発揮できる範囲を示してお’
) + Rt * Rtはtの値が大きいことにより縦
磁界効果が減少して電流しゃ断性能が低くなっている範
囲を示している。図かられかるように、tの値が小さい
と金属端板ヘアークが移行しやすいことから金属端板全
形成する材料への依存性が大きくなシ、一方tの値が大
きいと金属端板ヘアークが移行しないことから材料への
依存性はなくなる反面磁界の強さが支配する。また、固
定電極外径りが大きくなると磁界領域が広が5tの値を
若干大きくしてもよいことがわかる。電流しゃ断性能’
1loOチ発揮できるQl−Qlの範囲を表に示すと次
のようになる。In the figure, * p, a Pt indicates the range where the arc moves from the electrode 8 to the metal end plate 2 and the shearing performance is low due to the small value of t, and 5-Qx-Qt is the current Indicates the range in which shearing performance ft100'16 can be demonstrated.
) + Rt * Rt indicates a range in which the longitudinal magnetic field effect decreases due to a large value of t, and the current interrupting performance becomes low. As can be seen from the figure, when the value of t is small, the hair arc of the metal end plate is likely to migrate, so the dependence on the material that makes up the entire metal end plate is large, while when the value of t is large, the hair arc of the metal end plate is easy to migrate. Since there is no transition, there is no dependence on the material, but on the other hand, the strength of the magnetic field dominates. Furthermore, it can be seen that as the outer diameter of the fixed electrode increases, the magnetic field area expands and the value of 5t may be slightly increased. Current breaking performance'
The range of Ql-Ql that can exhibit 1loOchi is shown in the table below.
前記第2図及び表からもわかるように、tの範囲(を大
使]は、単一の片寄ったコイルにより縦磁界が印加され
ていることもあって、固定電極の外径りに依存すること
がわかる。そこでこれを換言すればsD−50mの場合
において i=+a15nはt−α3Dと表わすことが
でき、まft−D = 60 vmの場合においては、
tツ20gはt中α8Dと表わすことができる。したが
って、5US804Lを金属端板に用い九場合は2絽≦
t≦α3Dとすれば、1!流しゃ断性能即ちしゃ断能力
の高い真空インタラプタが得られる。As can be seen from Figure 2 and the table above, the range of t depends on the outer diameter of the fixed electrode, partly because the longitudinal magnetic field is applied by a single biased coil. Therefore, in other words, in the case of sD-50m, i=+a15n can be expressed as t-α3D, and in the case of ft-D=60 vm,
t20g can be expressed as α8D in t. Therefore, if 5US804L is used for the metal end plate, 2 絽≦
If t≦α3D, then 1! A vacuum interrupter with high flow interrupting performance, that is, high interrupting ability, can be obtained.
なお1本実施例では電極材料としてCu−耐火金属一鉄
族元索の組成からなりかつ粉末冶金法による複合材料、
即ちCu −Mo −Cr f用い次場合を示し九が、
耐火金属としてW−?Nbe用いるとともに鉄族元素と
してCo 、 F・、 Ni @用いても同様な効果が
得られる。tfe*cue耐火金属、鉄族元素の組成範
囲は電極材料として要求される猪条件を満足し得るよう
に決定されるが、 Cuは20〜80重量%、耐火金
属は5〜45重量%、鉄族元素は5〜45’!量チとす
るのがよい。In this example, the electrode material was a composite material composed of Cu-refractory metal monoiron group element and produced by powder metallurgy.
That is, using Cu-Mo-Cr f, the following case is shown.
W- as a refractory metal? A similar effect can be obtained by using Nbe as well as Co, F., and Ni@ as iron group elements. tfe*cue The composition range of refractory metals and iron group elements is determined to satisfy the boar conditions required for electrode materials, Cu is 20 to 80% by weight, refractory metals are 5 to 45% by weight, iron Group elements are 5-45'! It is best to use it in small quantities.
また、金属端板は一般にSUS 804 Lで作ってい
るが、これ以外のオーステナイト系のSUS材又はCu
、 F@、 F・−Ni −Co であっても同様
な効果が得られる。In addition, the metal end plates are generally made of SUS 804 L, but other austenitic SUS materials or Cu
, F@, F.--Ni--Co, similar effects can be obtained.
H1発明の効果
以上説明したように本発明によれば、固定電極と金属端
板との隙間f 2 wx以上でかつ固定電極外径寸法の
30%以下に設定してお夛、可動電極の外径寸法を固定
電極の外径寸法よシ大きくするとともに可動電極の背後
に緩和シールドを具えることによって極性効果及び電界
集中を防止したので。H1 Effects of the Invention As explained above, according to the present invention, the gap between the fixed electrode and the metal end plate is set to be greater than or equal to f 2 wx and less than 30% of the outer diameter of the fixed electrode, and the outer diameter of the movable electrode is The polarity effect and electric field concentration are prevented by making the diameter larger than the outer diameter of the fixed electrode and by providing a relaxation shield behind the movable electrode.
アークが固定電極から金属端板へ移行したC4るいはコ
イルによる縦磁界効果が減少したシせずしゃ断性能、耐
電圧性能つtりはしゃ断能力が向上する。The arc is transferred from the fixed electrode to the metal end plate, and the longitudinal magnetic field effect due to the coil is reduced, and the breaking performance, withstand voltage performance, and breaking ability are improved.
第1図は本発明による真空インタラプタの実施例の−m
を示す断面図、第2図は金属端板と固定電極との隙間を
変化させ九場合のしゃ断電流の相対値の大きさを示すグ
ラブ、第3図は真空容器の外周にコイルを具え九真空イ
ンタラプタの断面図。
第4図は第3図の真空インタラプタにおける電極径とし
ゃ断電流との関係を示すグラフ、第5図は第8図の真空
インタラプタにおける電極間ギャップと耐電圧との関係
を示すグラフ、第6図は固定電極を金属端板に接触させ
た縦磁界印加式の真空インタラプタの断面図、 ii!
7図は第6図の真空インクラックにおいて可動電極の外
径寸法を大きくした場合の等電位線の分布を示す説明図
、第8図は第6図の真空インタラプタにおいて可動電極
の外径寸法音大きくするとともに緩和シールドを具え九
場合の等電位線の分布を示す説明図、第9図(’) t
(blはその他の緩和シールドを示す断面図である。
1&・・・絶縁筒、1b・・・金属筒、2,8・・・金
属端板、4・・・真空容器、θ・・・固定リード捧、7
・・・可動リード俸、8・・・固定電極、9・・・可動
電極、 10・・・コイル、11・・・シールド、C・
・・コイルの内径寸法、t・・・固定電極と金属端板と
の隙間、D・・・固定電極の外径寸法。
第3図
鼻幣イ〕タラブク(lr)迷’7面膓
]シ盲411爬FIG. 1 shows an embodiment of the vacuum interrupter according to the present invention.
Figure 2 is a graph showing the relative magnitude of the cutoff current when the gap between the metal end plate and the fixed electrode is changed, and Figure 3 is a graph showing the relative magnitude of the cutoff current when the gap between the metal end plate and the fixed electrode is changed. A cross-sectional view of an interrupter. Fig. 4 is a graph showing the relationship between the electrode diameter and cutoff current in the vacuum interrupter shown in Fig. 3, Fig. 5 is a graph showing the relationship between the interelectrode gap and withstand voltage in the vacuum interrupter shown in Fig. 8, and Fig. 6 is a cross-sectional view of a vertical magnetic field application type vacuum interrupter with a fixed electrode in contact with a metal end plate, ii!
Figure 7 is an explanatory diagram showing the distribution of equipotential lines when the outer diameter of the movable electrode is increased in the vacuum ink crack of Figure 6, and Figure 8 is an explanatory diagram showing the distribution of the outer diameter of the movable electrode in the vacuum interrupter of Figure 6. Explanatory diagram showing the distribution of equipotential lines in the case of increasing the size and providing a relaxation shield, Figure 9 (') t
(bl is a sectional view showing other relaxation shields. 1 &... Insulating tube, 1b... Metal tube, 2, 8... Metal end plate, 4... Vacuum container, θ... Fixed Lead dedication, 7
...Movable lead salary, 8...Fixed electrode, 9...Movable electrode, 10...Coil, 11...Shield, C.
... Inner diameter dimension of the coil, t... Gap between the fixed electrode and metal end plate, D... Outer diameter dimension of the fixed electrode. Fig. 3 nose note I] Tarabuku (lr) '7-faced'] shiblindness 411 rep
Claims (1)
の内部に前記金属端板を貫通して相互に接近・離反可能
に固定リード棒及び可動リード棒を導入するとともに固
定リード棒、可動リード棒の内端部に夫々固定電極、可
動電極を固着しかつ固定電極側の金属端板の外側に縦磁
界発生コイルを具えた真空インタラプタにおいて、可動
電極の外径寸法を固定電極の外径寸法より大きく形成す
るとともに両電極を固定電極と同電位の金属部材で囲繞
して可動リード棒の外周面から可動電極の外周面までの
びる緩和シールドを具え、前記固定電極と固定側の前記
金属端板との隙間を2mm以上で前記固定電極の外径寸
法の30%以下に設定したことを特徴とする真空インタ
ラプタ。A fixed lead rod and a movable lead rod are introduced into a vacuum container formed by fixing metal end plates to both ends of an insulating cylinder so as to penetrate through the metal end plates so as to be able to approach and separate from each other, and a fixed lead rod; In a vacuum interrupter in which a fixed electrode and a movable electrode are fixed to the inner end of a movable lead rod, respectively, and a vertical magnetic field generating coil is provided on the outside of the metal end plate on the fixed electrode side, the outer diameter of the movable electrode is set to the outer diameter of the fixed electrode. A relaxation shield is formed larger than the diameter dimension and surrounds both electrodes with a metal member having the same potential as the fixed electrode, and extends from the outer circumferential surface of the movable lead rod to the outer circumferential surface of the movable electrode. A vacuum interrupter characterized in that a gap with an end plate is set to 2 mm or more and 30% or less of the outer diameter of the fixed electrode.
Priority Applications (8)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60134814A JPS61292830A (en) | 1985-06-20 | 1985-06-20 | Vacuum interruptor |
US06/865,895 US4661666A (en) | 1985-05-28 | 1986-05-21 | Vacuum interrupter |
CA000509860A CA1283151C (en) | 1985-05-28 | 1986-05-23 | Vacuum interrupter |
KR1019860004127A KR930011829B1 (en) | 1985-05-28 | 1986-05-27 | Vacuum breaker |
EP86107272A EP0204262B1 (en) | 1985-05-28 | 1986-05-28 | Vacuum interrupter |
IN396/CAL/86A IN165658B (en) | 1985-05-28 | 1986-05-28 | |
CN198686103785A CN86103785A (en) | 1985-05-28 | 1986-05-28 | Vacuum interrupter |
DE8686107272T DE3677640D1 (en) | 1985-05-28 | 1986-05-28 | VACUUM SWITCH. |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60134814A JPS61292830A (en) | 1985-06-20 | 1985-06-20 | Vacuum interruptor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61292830A true JPS61292830A (en) | 1986-12-23 |
JPH043048B2 JPH043048B2 (en) | 1992-01-21 |
Family
ID=15137115
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60134814A Granted JPS61292830A (en) | 1985-05-28 | 1985-06-20 | Vacuum interruptor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61292830A (en) |
-
1985
- 1985-06-20 JP JP60134814A patent/JPS61292830A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPH043048B2 (en) | 1992-01-21 |
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JPS6166324A (en) | Vacuum interrupter | |
JPS63236228A (en) | Vacuum interruptor | |
JPS593832A (en) | Vacuum interrupter | |
JP2881794B2 (en) | Magnetically driven electrodes for vacuum interrupters | |
JP2751300B2 (en) | Magnetically driven electrodes for vacuum interrupters | |
JPS59114716A (en) | Vacuum valve | |
JPS61245427A (en) | Vacuum siwtchgear | |
JPH04141926A (en) | Vacuum valve | |
JPS6345722A (en) | Vacuum valve | |
JPS6171519A (en) | Vacuum bulb | |
JPS6313219A (en) | Vacuum interruptor |