JPS60185320A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS60185320A
JPS60185320A JP3859884A JP3859884A JPS60185320A JP S60185320 A JPS60185320 A JP S60185320A JP 3859884 A JP3859884 A JP 3859884A JP 3859884 A JP3859884 A JP 3859884A JP S60185320 A JPS60185320 A JP S60185320A
Authority
JP
Japan
Prior art keywords
electrode
circuit breaker
contact
outer peripheral
vacuum
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
JP3859884A
Other languages
Japanese (ja)
Other versions
JPH0479090B2 (en
Inventor
黒沢 幸夫
岩下 喜代次
隆二 渡辺
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP3859884A priority Critical patent/JPS60185320A/en
Publication of JPS60185320A publication Critical patent/JPS60185320A/en
Publication of JPH0479090B2 publication Critical patent/JPH0479090B2/ja
Granted legal-status Critical Current

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  • 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】 〔発明の利用分野〕 本発明は主電極?改良した平行磁界型の真空遮断器に関
する。
[Detailed Description of the Invention] [Field of Application of the Invention] Is the present invention a main electrode? This invention relates to an improved parallel magnetic field type vacuum circuit breaker.

〔発明の背景〕[Background of the invention]

配電系統で多く使われている真空遮断器は、消弧性力が
非常に強く、小屯向遮断時に電流ケ突如零に急変させる
電流ざい断現象があり、変圧器やモータ回路では過大な
ザージ■圧を発生し易かった。そのため、従来は、この
過電圧から機器の絶縁ヶ保腹するためにコンデンサやア
レスター等のサージアブソーバが併用さt′15できて
いる。しかし、サージアブソーバは真空遮断器の犬@な
利点である小形性ケ損う。これに対処するため、サージ
アブソーバを省略するには、電流さい断現象ケ生ずる電
流レベル?下げる必要がありこれは、電極材料で決せる
Vacuum circuit breakers, which are often used in power distribution systems, have a very strong arc-extinguishing force, and there is a current rupture phenomenon in which the current suddenly changes to zero when the circuit is shut off in the small direction. ■It was easy to generate pressure. Therefore, conventionally, surge absorbers such as capacitors and arresters have been used in combination to insulate and protect equipment from this overvoltage. However, surge absorbers lose the advantage of vacuum circuit breakers, namely their small size. To deal with this, how can I omit the surge absorber due to the current level that causes the current cutting phenomenon? This can be determined by the electrode material.

さい断電流レベルの小さい電極材料どしては、コバルト
(CO)、銀(Ag)並びにセレン(Se)等の複合材
がある。複合屯健材料?平行磁界型の主電極に使用する
と、主電極は電極基板に無酸化鋼ケ、電極基板に隣接し
てco、Ag。
Examples of electrode materials with low cutting current levels include composite materials such as cobalt (CO), silver (Ag), and selenium (Se). Composite tunken material? When used in a parallel magnetic field type main electrode, the main electrode has an electrode substrate made of non-oxidized steel, and adjacent to the electrode substrate made of Co, Ag.

Seから成る接触層を使用し、両者はろう付たとえばA
gロー付金して一体にする。[7か(、、Beが入って
いるのでろう付は性が悪い。そのため、Co基板ケ接触
層のCo −A g −S e材の製造時に焼結にて付
けておき電極基板との間に配置[−だザンドイツテ状に
して、ろう付けをすることが考えられる。
A contact layer consisting of Se is used, and the two are brazed, e.g.
G-braze it and make it into one piece. [7] Because it contains Be, the brazing properties are poor.Therefore, when manufacturing the Co-Ag-Se material for the contact layer of the Co substrate, it is attached by sintering and the contact layer between the electrode and the substrate is It is conceivable to place it in a Zandermante shape and braze it.

しかし、主電極にCo基板ケ使用すると、C。However, when a Co substrate is used as the main electrode, C.

基板は強磁性体であるため、磁気シールドとなって【〜
捷っで、電極間空間に有効な平行磁界音発生することが
できない。
Since the substrate is ferromagnetic, it acts as a magnetic shield and
Due to this, effective parallel magnetic field sound cannot be generated in the space between the electrodes.

また、主電極中央の接点部の尚さ寸法?外周部のそれよ
りより尚く構成し、更にさい断電流レベルケ改善した主
電極では、CC01A、並びにSeからなる電極材料ケ
接点部だけに限ると、Co、Ag並びにSeからなる電
極材料は、アーク電圧が約12Vと1、一般用真空遮断
器用電極材料たとえば銅(Cu)−ビスマス(Bi)(
c−使用した外周部は、アーク電圧17−20Vである
ため、接点部からその外周部の主電極表面へのアークの
移転が出来ず、アークは接点部だけに集中し〜て[7甘
い良好な遮断性能?得ることかで@ない。
Also, what is the size of the contact part at the center of the main electrode? In the main electrode, which is constructed more than that of the outer circumferential part and has an improved cutting current level, the electrode material is made of CC01A and Se.Limiting to the contact part, the electrode material made of Co, Ag and Se is used to prevent arcing. The voltage is about 12V, and the electrode material for general vacuum circuit breakers, such as copper (Cu)-bismuth (Bi) (
c- Since the arc voltage of the outer circumferential part used was 17-20V, the arc could not be transferred from the contact part to the main electrode surface of the outer circumferential part, and the arc was concentrated only on the contact part. What is the blocking performance? It's not about getting it.

このようなところから、従来、さい断電流の小さい大電
流線断用の真空遮断器は不ロJ能祝されていた。
For this reason, vacuum circuit breakers for large current line breaks with small breaking currents have traditionally been rejected.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、さい断′屯ofレベルが低くてサージ
アブソーバケ不要とでき、かつ25 k A以上の大m
I&遮断に好適な真空遮断器?提供することにある。
The object of the present invention is to have a low cutting force level, which eliminates the need for a surge absorber, and which has a large molar capacity of 25 kA or more.
Is a vacuum circuit breaker suitable for I&C? It is about providing.

〔発明の概要〕[Summary of the invention]

本発明の主′U4L極は、中火部にコバルト、銀並びに
セレンより成る接点部と、接点部の周囲にコ/くルト、
銀並びにテルルエリ成る外周部と、から構成することに
より、上記目的ケ達成することにある。
The main 'U4L pole of the present invention has a contact part made of cobalt, silver, and selenium in the medium heat part, and a cobalt/coat part around the contact part.
The above object is achieved by comprising an outer peripheral portion made of silver and tellurium.

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

以下、本発明の実施例?第1図に示す真空遮断器lによ
り説明する。
Below are examples of the present invention? This will be explained using a vacuum circuit breaker l shown in FIG.

真空箱断器1は、絶縁円筒2並びに端板3,4工りなる
真空容器内に、導電棒6.7が端板3゜4ヶ貫通して設
けられ、一対の電極8,9が夫々、真空容器内で導電棒
6.HC固着されて構成されている。一方の導電棒7は
ベローズ10i介して端板4に気密に封着されている。
The vacuum box disconnector 1 is provided with a conductive rod 6.7 passing through four end plates 3° in a vacuum container consisting of an insulating cylinder 2 and end plates 3 and 4, and a pair of electrodes 8 and 9, respectively. , conductive rod 6. in a vacuum container. It is made up of HC fixed. One conductive rod 7 is hermetically sealed to the end plate 4 via a bellows 10i.

4電棒6は端板3に直接取り付けられ気密に封着きれて
いる。可動側および固定1!l電極8,9は、これらケ
取り囲んで配置された円筒状の金属蒸気シールド11が
、シールド支え12によって、絶縁円筒2の中間部に取
着されている。図示していない操作機構により導電棒7
が軸方向上側に駆動されることにより。
The four electric rods 6 are directly attached to the end plate 3 and hermetically sealed. Movable side and fixed 1! A cylindrical metal vapor shield 11 surrounding the l electrodes 8 and 9 is attached to the middle part of the insulating cylinder 2 by a shield support 12. The conductive rod 7 is operated by an operation mechanism (not shown).
is driven upward in the axial direction.

可動側電極8は同定側電極9に接触し、真空遮断器は閉
路状態となり、導電棒7が軸方向下4ii1に駆動され
ることにより、固定側電極9より可動側電極8が離れて
真空遮断器は、開路状態へと移る。
The movable side electrode 8 comes into contact with the identification side electrode 9, the vacuum circuit breaker becomes a closed circuit state, and as the conductive rod 7 is driven axially downward 4ii1, the movable side electrode 8 separates from the fixed side electrode 9 and the vacuum is interrupted. The device moves to the open circuit state.

これらの電極8.91dコイル電極13、主電極14と
から構成されているが、両電極の構造が同じなので、固
定側電極8の説明?省略し、可動側電極9について第2
図に工り説明する。
These electrodes 8.91d are composed of a coil electrode 13 and a main electrode 14, but since the structure of both electrodes is the same, what is the explanation for the fixed side electrode 8? omitted, and the second for the movable electrode 9.
This will be explained using the diagram.

コイル電極13は裏面に導電棒7ケ固着した中心1fi
l15に、中心部より外周方向に延びる腕部16ケ取付
け、腕部16より中心部15(I−包囲するように円周
方向に延び、かつ他端が間隙17と対応している外周部
18(r、腕部16に一体に形成している。接続部19
は外周部他端に設けられ、かつ主電極14に電気的に接
続している。
The coil electrode 13 has a center 1fi with 7 conductive rods fixed to the back surface.
16 arms extending from the center to the outer circumferential direction are attached to l15, and the arm 16 is attached to the center part 15 (I- an outer circumferential part 18 which extends in the circumferential direction so as to surround it and whose other end corresponds to the gap 17). (r, integrally formed in the arm portion 16. Connection portion 19
is provided at the other end of the outer periphery and is electrically connected to the main electrode 14.

主電極14は外周側から中心側に向って8本の直線状の
スリット20ケ形成している。スリット20は導電棒7
からの電流がコイル電極13を流れて、接続部19に介
して主電極14のアーク100に流れと、コイル電極1
3で平行磁界(図示せず)4発生する。平行磁界が主電
極14ケ印加すると、主電極14にうず電が流れるが、
スリット20によりうず電流ケ小さくできる。このため
、うず電流によるイ磁界によって、平行磁界が減極され
るの?少なくで〜きる。
The main electrode 14 has 20 eight linear slits extending from the outer periphery toward the center. The slit 20 is the conductive rod 7
The current flows through the coil electrode 13 and flows through the connection 19 to the arc 100 of the main electrode 14 and the coil electrode 1
3, a parallel magnetic field (not shown) 4 is generated. When a parallel magnetic field is applied to the 14 main electrodes, eddy currents flow in the main electrodes 14,
The eddy current can be reduced by the slit 20. For this reason, does the parallel magnetic field become depolarized by the magnetic field caused by the eddy current? You can do it with less.

主電極14の構造は、第3図に示す如く、電極基板2ま
たとえば無酸化銅の一端は、接続部19に接続し、他端
はCo基板22ケ介して接点部23および接点部を包囲
する外周部24と?ろう付けにより一体に固着している
。接点部23け第4図に示すように中心に中心溝25ケ
有するリング状の接点部23Aに形成してもよい。接点
部23の高さ寸法は外周部24のそれより高く、接点部
23の電極材料は、Co、Ag並びにSeにより構成し
ている。接点部23の成分範囲は、Co用:20〜80
(%)、Ag惜13〜50(刑、S e it、t 7
〜30(%)の範囲内にて構成している。
As shown in FIG. 3, the structure of the main electrode 14 is such that one end of the electrode substrate 2, for example, non-oxidized copper, is connected to the connecting portion 19, and the other end surrounds the contact portion 23 and the contact portion via the Co substrate 22. With the outer peripheral part 24? They are fixed together by brazing. As shown in FIG. 4, the contact portion 23 may be formed into a ring-shaped contact portion 23A having 25 central grooves in the center. The height of the contact portion 23 is higher than that of the outer peripheral portion 24, and the electrode material of the contact portion 23 is made of Co, Ag, and Se. The component range of the contact part 23 is for Co: 20 to 80
(%), Ag 13-50 (punishment, S e it, t 7
It is comprised within the range of ~30(%).

外周部24の′電極材料は、Co、Ag並びにTe(テ
ルル)により構成しでいる。外周部の成分範囲は、Co
−1720〜80(%)、Ag it l 8〜72(
%)、T e i:5〜22 (%)の範囲内にて構成
されている。
The electrode material of the outer peripheral portion 24 is made of Co, Ag, and Te (tellurium). The component range at the outer periphery is Co
-1720~80(%), Agit l 8~72(
%), T e i: 5 to 22 (%).

この主電極14の構成によれば、Co基板22は接点部
23だけに限られ、Co基板22の磁気シールド効果は
少なく、電極間空間の大部分の領域は、外周部24には
有効な平行磁界音発生できる。一方、接点部23ど外周
部24どのアーク電圧(V)−:、第5図(A)に示す
ように、両者ともほぼ等(−い。このため、接点部23
に点弧したアーク100は、スムーズに外周部24に移
り、接点部23ケ溶損することなく、[−や断性能ケ向
」二することができる。
According to this configuration of the main electrode 14, the Co substrate 22 is limited to the contact portion 23, the magnetic shielding effect of the Co substrate 22 is small, and most of the inter-electrode space is effectively parallel to the outer peripheral portion 24. Can generate magnetic field sound. On the other hand, as shown in FIG.
The arc 100 ignited smoothly moves to the outer peripheral portion 24, and the contact portion 23 is not melted and damaged, and the arc 100 can be improved.

捷た、接点部23と外周部24とのざい断電流(I)は
、第5図(B)に示す如く、外周部24の方が接点部2
3より多少大きい。このため、遮断時に、外周部24に
点弧しているアーク100は、接点部23工り早く消弧
する。それは、Teの蒸気圧がSeのそれより低(、T
e1j:Seより早く蒸発するから、アーク100は接
点部23より早く外周部23で消弧した後、接点部23
″′Cア一ク1ooi点弧しているので、電流零点又は
電流零点附近で消弧する。このため、第5図FB)に示
すように86のさい断電流I(WA、)は、Teのそれ
より小さいので、サージ電圧(V)?小さくできる。し
たがって、本発明では従来のサージアブソーバを使用す
る必要が無くなったので、真空遮断器ケ小型化できる。
As shown in FIG. 5(B), the rupture current (I) between the contact portion 23 and the outer peripheral portion 24 is higher in the outer peripheral portion 24 than in the contact portion 2.
Slightly larger than 3. Therefore, the arc 100 ignited in the outer circumferential portion 24 at the time of interruption is quickly extinguished by the contact portion 23. It is because the vapor pressure of Te is lower than that of Se (, T
e1j: Since it evaporates faster than Se, the arc 100 is extinguished at the outer peripheral part 23 earlier than the contact part 23, and then
Since the current is ignited, the current is extinguished at or near the current zero point. Therefore, as shown in FIG. Since the surge voltage (V) can be reduced, the present invention eliminates the need to use a conventional surge absorber, making it possible to downsize the vacuum circuit breaker.

この実施例で腕部、外周部から成る4個の磁界発生部で
は、同方向の平行磁界音発生するコイル電極ケ使用(ま
たが、4個の磁界発生部のうち対象的に配置された2個
づつが異なる方向の平行磁界?発生するコイル電極葡使
用[−たり、或いは真空容器の外側コイル巻回したコイ
ル電極等?使用してもよい。
In this embodiment, the four magnetic field generating parts consisting of the arm part and the outer peripheral part use coil electrodes that generate parallel magnetic field sound in the same direction (also, two symmetrically arranged magnetic field generating parts of the four magnetic field generating parts A coil electrode may be used which generates parallel magnetic fields in different directions, or a coil electrode may be used which is wound around a coil outside the vacuum container.

〔発明の効果〕 以上のように、本発明の真空遮断器によれば、発生サー
ジは小さくザージアブソーバ?不要になり、真空遮断器
を小形化できる。
[Effects of the Invention] As described above, according to the vacuum circuit breaker of the present invention, the generated surge is small. This is no longer necessary and the vacuum circuit breaker can be made smaller.

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

第1図は本発明の実施例として示した真空遮断器の側断
面図、第2図は第1図に使用した可動側電極の斜視図、
第3図は第2図の側断面図、第4図は他の実施例として
電極の側断面図、第5図(A)および(B)はアーク電
圧およびさい断電流の特性図である。 2・・・真空容器、8および9・・・固定側および可動
側電極、13・・・コイル電極、14・・・主電極、2
3・・・接点部、24・・・外周部。
FIG. 1 is a side sectional view of a vacuum circuit breaker shown as an embodiment of the present invention, FIG. 2 is a perspective view of the movable side electrode used in FIG. 1,
3 is a side sectional view of FIG. 2, FIG. 4 is a side sectional view of an electrode as another example, and FIGS. 5(A) and 5(B) are characteristic diagrams of arc voltage and cutting current. 2... Vacuum vessel, 8 and 9... Fixed side and movable side electrodes, 13... Coil electrode, 14... Main electrode, 2
3...Contact part, 24...Outer peripheral part.

Claims (1)

【特許請求の範囲】 1、真空容器内に接離自在な少なくとも一対の圧電極?
配置し、主電極に平行磁界ケ印加する真空遮断器におい
て、上記主電極は中央部にコバルト、銀並びにセレンエ
リ成る接点部と、接点部の周囲にコバルト、銀並びにテ
ルルより成る外周部と、から構成することケ特徴とする
真空遮断器。 2、上記主電極は電極基板上に上記接点部および外周部
?配置L %外周部と電極基板との間および接点部と電
極基板との間にコバルト層を介して、それぞれろう付け
より一体に構成することを特徴とする特許請求の範囲第
1項記載の真空遮断器。 3、接点部の高さ寸法?外周部のそれより高く構成する
ことケ特徴とする1特許請求の範囲第1項又は第2項記
載の真空遮断器。
[Claims] 1. At least one pair of piezo electrodes that can be freely brought into contact and separated from the vacuum container?
In a vacuum circuit breaker which applies a parallel magnetic field to the main electrode, the main electrode has a contact part made of cobalt, silver and selenium in the center, and an outer peripheral part made of cobalt, silver and tellurium around the contact part. Vacuum circuit breaker with features: 2. Does the main electrode have the contact part and outer peripheral part on the electrode substrate? Arrangement L % The vacuum according to claim 1, characterized in that the outer circumferential portion and the electrode substrate are integrally formed by brazing each other with a cobalt layer interposed between the contact portion and the electrode substrate. circuit breaker. 3. What is the height of the contact part? The vacuum circuit breaker according to claim 1 or 2, characterized in that the vacuum circuit breaker is constructed higher than that of the outer peripheral portion.
JP3859884A 1984-03-02 1984-03-02 Vacuum breaker Granted JPS60185320A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3859884A JPS60185320A (en) 1984-03-02 1984-03-02 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3859884A JPS60185320A (en) 1984-03-02 1984-03-02 Vacuum breaker

Publications (2)

Publication Number Publication Date
JPS60185320A true JPS60185320A (en) 1985-09-20
JPH0479090B2 JPH0479090B2 (en) 1992-12-15

Family

ID=12529711

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3859884A Granted JPS60185320A (en) 1984-03-02 1984-03-02 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS60185320A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04368733A (en) * 1991-06-17 1992-12-21 Mitsubishi Electric Corp Vacuum switch tube
JP2003092221A (en) * 2001-09-17 2003-03-28 Densei Lambda Kk Inductance component
JP2014116183A (en) * 2012-12-10 2014-06-26 Toshiba Corp Vacuum valve

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04368733A (en) * 1991-06-17 1992-12-21 Mitsubishi Electric Corp Vacuum switch tube
JP2003092221A (en) * 2001-09-17 2003-03-28 Densei Lambda Kk Inductance component
JP2014116183A (en) * 2012-12-10 2014-06-26 Toshiba Corp Vacuum valve

Also Published As

Publication number Publication date
JPH0479090B2 (en) 1992-12-15

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