JPS585929A - Electrode for vacuum breaker - Google Patents

Electrode for vacuum breaker

Info

Publication number
JPS585929A
JPS585929A JP10341081A JP10341081A JPS585929A JP S585929 A JPS585929 A JP S585929A JP 10341081 A JP10341081 A JP 10341081A JP 10341081 A JP10341081 A JP 10341081A JP S585929 A JPS585929 A JP S585929A
Authority
JP
Japan
Prior art keywords
electrode
contact
arc
contact portion
damper
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
JP10341081A
Other languages
Japanese (ja)
Inventor
岩下 喜代次
黒沢 幸夫
和田 昭
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 JP10341081A priority Critical patent/JPS585929A/en
Publication of JPS585929A publication Critical patent/JPS585929A/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】 本発明は真空しゃ断器用電極に係り、特に通電性能を高
め短時間電流通電での溶着を阻止するに好適な電極構造
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrode for a vacuum breaker, and particularly to an electrode structure suitable for improving current carrying performance and preventing welding during short-time current passing.

第1図に示す真空しゃ断器Vよ、端子板3,4と絶縁筒
2、ベローズ5で真空容器IA’に作り、その中には固
定ホルダー7に固着した固定電極6と、可動ホルダー9
に固着した可動電極8および中間シールド10が設けら
れている。
The vacuum breaker V shown in FIG. 1 is made into a vacuum container IA' with terminal plates 3 and 4, an insulating tube 2, and a bellows 5, and inside it is a fixed electrode 6 fixed to a fixed holder 7 and a movable holder 9.
A movable electrode 8 and an intermediate shield 10 are provided which are fixed to the.

これら両電極はしゃ断性能を向上させるためアークと平
行な磁界を発生する平行磁界形電極を用いる例が多くな
っている。その構造は第2図に示すようにアークが発生
、消弧するアーク電極11、アーク電極11の機械強度
を増す働きをする補強板12、電流を円周方向に流すコ
イル電極13、補強板12を支えると共にホルダー9か
らアーク電極11に流れ込む電流を制限する抵抗体14
から成っている。これらの各部品は第3図の矢印15の
方向に重ね合わせ、お互いの接触部を接合することによ
り第2図の構造が得られる。
In order to improve the breaking performance of these electrodes, parallel magnetic field type electrodes that generate a magnetic field parallel to the arc are increasingly used. As shown in Fig. 2, its structure includes an arc electrode 11 that generates and extinguishes an arc, a reinforcing plate 12 that increases the mechanical strength of the arc electrode 11, a coil electrode 13 that allows current to flow in the circumferential direction, and a reinforcing plate 12. A resistor 14 that supports the holder 9 and limits the current flowing from the holder 9 to the arc electrode 11.
It consists of The structure shown in FIG. 2 is obtained by overlapping each of these parts in the direction of arrow 15 in FIG. 3 and joining their contact parts.

各部全流れる電流工は、第3図に示すように、ホルダー
9からコイル電極13の中心部に達したあと、コイル電
極13の円周部を流れ、突起部13bからアーク電極1
1に流れ込む。アーク電極11では溝188〜18dで
制限されるため半径方向にのみ流れて接触部11aに至
る。この時の電流通路をアーク電極11側から見ると第
4図の点線で示したようになり、アーク電極11の表面
に4領域に分れてアークと平行な磁界Hが発生する。接
触部11aにアーク16が発生すると、第4図に示した
ように磁界の非常に弱い中心付近から磁界の強い4領域
にひろがり、そこで消弧される。
As shown in FIG. 3, the electric current flowing through each part flows from the holder 9 to the center of the coil electrode 13, flows around the circumference of the coil electrode 13, and flows from the protrusion 13b to the arc electrode 13.
Flows into 1. Since the arc electrode 11 is restricted by the grooves 188 to 18d, it flows only in the radial direction and reaches the contact portion 11a. When viewed from the arc electrode 11 side, the current path at this time is as shown by the dotted line in FIG. 4, and a magnetic field H parallel to the arc is generated on the surface of the arc electrode 11 in four areas. When an arc 16 is generated in the contact portion 11a, it spreads from near the center where the magnetic field is very weak to four areas where the magnetic field is strong, as shown in FIG. 4, and is extinguished there.

平行磁界形電極は上述の通りアークを電極全面にひろけ
て局部的な溶融を防ぎ、しゃ断性能金高めていることに
あるが、このような電極でも材料によ、つて性能が左右
されるのは避けられない。すなわち、アーク電極11の
材料にCLl −P b合金やCLI−Br合金などを
用いれば、電流通電時においては、これらの合金は比較
的軟らかい材料であることから、電極接触部11aでは
師接触となり易く、かつ導電率も高いために通電性能が
優れている。しかし、これらの合金は融点も低いために
アークが発生すると電極表面が溶け、多量の金属蒸気を
生じてしゃ断不能し易くなる。また材料をCu−pe、
 Cu−coなどの合金にした場合、これらの材料は耐
アーク、耐電圧性能に優れているため40kAや63k
A  といった大きな電流をしゃ断できるが、これらの
材料は硬いため、わずかの偏心があると大きな接触力を
与えても変形しにくいため片当りとなり、電極接触部1
1aでは点接触となり易く、またこれらの合金は導電率
も比較的小さいため性能試験規格に沿って40kAや6
3kAといった大きな電流を通電すると発熱が著しく、
最悪の場合には接触部11aが溶けて溶着し、可動電極
8が固定電極6から離れなくなってしまう現象が発生す
る。したがって、CLJ−pb程度に軟らかく、耐アー
ク性能が(:’ u −CO合金と同じような材料があ
れば問題ないが、実際には両方を満足する材料はなく、
通電性能としゃ断性能の両者を同時に十分に満足できな
かった。
As mentioned above, parallel magnetic field type electrodes spread the arc over the entire surface of the electrode to prevent local melting and improve the breaking performance, but even with such electrodes, the performance is affected by the material used. is unavoidable. In other words, if a CLl-Pb alloy or a CLI-Br alloy is used as the material for the arc electrode 11, since these alloys are relatively soft materials when current is applied, there will be no contact at the electrode contact portion 11a. Because it is easy to use and has high conductivity, it has excellent current carrying performance. However, since these alloys have low melting points, when an arc occurs, the electrode surface melts and a large amount of metal vapor is generated, making it difficult to shut off. Also, the material is Cu-pe,
When made into alloys such as Cu-co, these materials have excellent arc resistance and withstand voltage performance, so
Although large currents such as A can be interrupted, these materials are hard, so if there is a slight eccentricity, they will not easily deform even if a large contact force is applied, resulting in uneven contact, and the electrode contact part 1
1a tends to cause point contact, and these alloys also have relatively low electrical conductivity, so in line with performance test standards, 40 kA and 6
When a large current such as 3kA is applied, heat generation is significant.
In the worst case, a phenomenon occurs in which the contact portion 11a melts and welds, and the movable electrode 8 becomes unable to separate from the fixed electrode 6. Therefore, there is no problem if there is a material that is as soft as CLJ-pb and has similar arc resistance (:' u -CO alloy, but in reality there is no material that satisfies both.
It was not possible to fully satisfy both current carrying performance and breaking performance at the same time.

本発明の目的は、通電性能としゃ断性能の両者とも優れ
た電極の真空しゃ断器用電極を提供することにある。
An object of the present invention is to provide an electrode for a vacuum breaker that is excellent in both current carrying performance and breaking performance.

本発明の電極は、しゃ断性能を上げるためには、アーク
電極にCu−Co系合金などのような融点の高い材料が
用いられるが、これらの材料は硬く、アーク電極の接触
部では片当りなどによって点接触となり易い。接触部を
面接触に近い状態を得るためには、接触部か、その他の
部分で接触部が面接触に近い状態が得られるように変形
すれば良い。
In order to improve the breaking performance of the electrode of the present invention, a material with a high melting point such as a Cu-Co alloy is used for the arc electrode, but these materials are hard and cause uneven contact at the contact part of the arc electrode. Point contact is likely to occur. In order to obtain a state close to surface contact at the contact portion, the contact portion or other portions may be deformed so as to obtain a state close to surface contact.

このことから接触部の裏側に軟かく変形し易い材料を用
いれば、上記問題を解決できる。
Therefore, the above problem can be solved by using a soft and easily deformable material on the back side of the contact portion.

以下、本発明の一実施例を第5図にて説明する。An embodiment of the present invention will be described below with reference to FIG.

第5図は可動電極19で、アーク電極20と接触部20
aにはCu−Co合金のような耐アーク性能の、優れた
材料を用いアーク電極20と接触部20aとの間に(:
’u−pb合金やAg合金のような軟らかく、かつ導電
率の大きいダンパー電極21を配置した。
FIG. 5 shows the movable electrode 19, the arc electrode 20 and the contact part 20.
A is made of a material with excellent arc resistance such as a Cu-Co alloy between the arc electrode 20 and the contact part 20a (:
A damper electrode 21 that is soft and has high conductivity, such as a u-pb alloy or an Ag alloy, is arranged.

ダンパー電極21を配置すれば、偏心などで接触部20
aが片当りを起こしても、アーク電極20と接触部20
aとの間にはさまれたダンパー電極21が変形し、接触
部20aでは面接触に近い状態が得られる。したがって
、接触部20aが硬く、若干導電率が低い材料であって
も接触部20aが面接触となるために、通電面積が大き
くなり、接触部20aでの温度上昇が緩和されるため、
通電時接触部が溶けて溶着するということがない。この
ように、接触部20aの裏側にダンパル電極21を設け
たことにより、接触部20aは常に面接触を保つことが
できるために、通電性能が良く、また電極材に耐アーク
性能の良い材料を用いることができるので、通電、しゃ
断の両性能を優れたものにすることができる。
If the damper electrode 21 is placed, the contact portion 20
Even if a causes uneven contact, the arc electrode 20 and the contact part 20
The damper electrode 21 sandwiched between the contact portion 20a and the contact portion 20a is deformed, and a state close to surface contact is obtained at the contact portion 20a. Therefore, even if the contact part 20a is made of a material that is hard and has a slightly low conductivity, the contact part 20a forms a surface contact, so the current-carrying area becomes large, and the temperature rise at the contact part 20a is alleviated.
There is no chance of the contact parts melting or welding when energized. In this way, by providing the damper electrode 21 on the back side of the contact part 20a, the contact part 20a can always maintain surface contact, so it has good current carrying performance, and the electrode material is made of a material with good arc resistance. Since it can be used, it is possible to improve both the current conduction and cutoff performance.

上述では、接触部20aの径とダンパー電極の径を一致
したものとしたが、必ずしも一致させる必要はなく、第
6図のようにダンパー電極の径を小さくしても第7図や
第8図のようにダンパー電極21、又はダンパー電極2
1と接触部20aの両刀に複数の溝22を設けたもので
も上記と同じ効果が得られる。
In the above description, it is assumed that the diameter of the contact portion 20a and the diameter of the damper electrode are the same, but they do not necessarily have to be the same, and even if the diameter of the damper electrode is made smaller as shown in FIG. Damper electrode 21 or damper electrode 2 as in
The same effect as described above can also be obtained by providing a plurality of grooves 22 on both the blades of the contact portion 1 and the contact portion 20a.

以上のように本発明によれば、接触部の裏側に容易に変
形し易い材料でできたダンパー電極を配置したことによ
り、片当りが起ってもダンパー電極が変形して、接触部
は常に面接触に近い状態を得ることができるので、局部
的に溶融することがなく、耐溶着性を得ることができる
。したがって、通電性能としゃ断性能とに優れた電極を
提供できる。
As described above, according to the present invention, by arranging the damper electrode made of an easily deformable material on the back side of the contact part, the damper electrode is deformed even if uneven contact occurs, and the contact part is always Since it is possible to obtain a state close to surface contact, there is no local melting, and welding resistance can be obtained. Therefore, it is possible to provide an electrode with excellent current conduction performance and cutoff performance.

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

第1図は従来の真空しゃ断器の側断面図、第2図は従来
の電極の側断面図、第3図はその分解斜視図、第4図は
磁界の状況説明図、第5図は本発明の電極の側断面図、
第6図は本発明の他の実施例を示すアーク電極部分の側
断面図、第7図、第8図、は本発明の他の実施例として
示した電極の斜視図である。 20・・アーク電極、21・・・接触部、21・・・ダ
ンパー電極、22a〜22h・・・溝。 馬 II!I も 3 口 第 5 口 第“口      策、7い ′Jj、8  口
Fig. 1 is a side sectional view of a conventional vacuum breaker, Fig. 2 is a side sectional view of a conventional electrode, Fig. 3 is an exploded perspective view thereof, Fig. 4 is an explanatory diagram of the state of the magnetic field, and Fig. 5 is a booklet. A side sectional view of the electrode of the invention,
FIG. 6 is a side sectional view of an arc electrode portion showing another embodiment of the invention, and FIGS. 7 and 8 are perspective views of electrodes shown as other embodiments of the invention. 20... Arc electrode, 21... Contact portion, 21... Damper electrode, 22a to 22h... Groove. Horse II! I also 3rd mouth 5th mouth "mouth plan, 7'Jj, 8th mouth"

Claims (1)

【特許請求の範囲】[Claims] 1、真空容器内に収納した外部に延びるホルダーを有す
る接離自在な一対の電極と、上記電極の対応面より他方
の電極側に突出する接触部とから成る真空しゃ断器にお
いて、上記接触部と電極との間にダンパー電極を設ける
ことを特徴とする真空しゃ断器用電極。
1. A vacuum breaker consisting of a pair of electrodes that are housed in a vacuum container and have a holder that extends to the outside and that can be freely brought into and out of contact with the other electrode, and a contact portion that protrudes from the corresponding surface of the electrode toward the other electrode, in which the contact portion and An electrode for a vacuum breaker, characterized in that a damper electrode is provided between the electrode and the damper electrode.
JP10341081A 1981-07-03 1981-07-03 Electrode for vacuum breaker Pending JPS585929A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10341081A JPS585929A (en) 1981-07-03 1981-07-03 Electrode for vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10341081A JPS585929A (en) 1981-07-03 1981-07-03 Electrode for vacuum breaker

Publications (1)

Publication Number Publication Date
JPS585929A true JPS585929A (en) 1983-01-13

Family

ID=14353277

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10341081A Pending JPS585929A (en) 1981-07-03 1981-07-03 Electrode for vacuum breaker

Country Status (1)

Country Link
JP (1) JPS585929A (en)

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