JPS5868819A - Electrode for vacuum breaker - Google Patents

Electrode for vacuum breaker

Info

Publication number
JPS5868819A
JPS5868819A JP16708081A JP16708081A JPS5868819A JP S5868819 A JPS5868819 A JP S5868819A JP 16708081 A JP16708081 A JP 16708081A JP 16708081 A JP16708081 A JP 16708081A JP S5868819 A JPS5868819 A JP S5868819A
Authority
JP
Japan
Prior art keywords
electrode
arc
performance
arc electrode
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.)
Pending
Application number
JP16708081A
Other languages
Japanese (ja)
Inventor
和田 昭
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 JP16708081A priority Critical patent/JPS5868819A/en
Publication of JPS5868819A publication Critical patent/JPS5868819A/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のしゃ断部になる真空バルブの電
極に係り、特にアークと平行な磁界を発生する手段を備
えてなる電極に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrode of a vacuum valve serving as a breaking section of a vacuum breaker, and particularly to an electrode provided with means for generating a magnetic field parallel to an arc.

真空バルブのしゃ断性能を向上させるためのアークと平
行な磁界を発生する電極、すなわち平行磁界形′i′を
極を用いる例が多くなっているが、その真空バルブ1の
構造はg1図のようになっている。
In order to improve the breaking performance of a vacuum valve, there are many examples of using electrodes that generate a magnetic field parallel to the arc, that is, parallel magnetic field type 'i' poles, and the structure of the vacuum valve 1 is as shown in diagram g1. It has become.

第1図において1は真空バルブで絶縁m 2 、rg子
板3,4、ベローズ5で密封容器を作り、その中には固
定ホルダ7に取り+iけた固定電極6、可動ホルダ9に
取り付けた可動電極8が配置されている。10は固定電
極6および可動電極8から電気的に絶縁されている中間
シールドである。固Y電極6と可動電極8は同一構造の
もので、たとえば、可動電極8は第2図に示すようにア
ークが発生、消弧するアーク′醒極11、′直流を円周
方向にも流してコイルの役目をするコイル電極12、お
よび可動ホルダ9からなっている。
In FIG. 1, 1 is a vacuum valve, and a sealed container is made of an insulator m 2 , RG platelets 3 and 4, and a bellows 5. Inside the container, there is a fixed electrode 6 attached to a fixed holder 7, and a movable one attached to a movable holder 9. Electrodes 8 are arranged. 10 is an intermediate shield electrically insulated from the fixed electrode 6 and the movable electrode 8. The fixed Y electrode 6 and the movable electrode 8 have the same structure.For example, as shown in FIG. It consists of a coil electrode 12 that functions as a coil, and a movable holder 9.

これらの各部品は第3図の矢印13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。
The structure shown in FIG. 2 is obtained by overlapping each of these parts in the direction of arrow 13 in FIG. 3 and joining their contact parts.

谷部を流れる電流も第3図に示しである。すなわち、ホ
ルダ9からコイル電極12の中心部に達したあと、約半
分ずつの電流が2方向に分れでコイル電極12の円周部
に行き、寸だ、その各々の電流が2分されて円周部を流
れてコイル電−12の突起部12a、121)からアー
ク電極11に流れ込む。アーク亀ポ11では@16で制
限されるため半径方向]、5a、15b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
から見るとg4図実線で示したようになり、アーク電極
11の入面に4領域に分れてアークと平行な磁界が発生
する。もし、接触部11aにアーク14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1・]近か
ら磁界の強い4頭」或にひろがり、そこで消弧される。
The current flowing through the valley is also shown in FIG. In other words, after reaching the center of the coil electrode 12 from the holder 9, approximately half of the current is divided into two directions and goes to the circumference of the coil electrode 12, and each current is divided into two. It flows around the circumference and flows into the arc electrode 11 from the protrusions 12a, 121) of the coil electrode 12. Since the arc point 11 is restricted by @16, it flows only in the radial direction], 5a, and 15b, and reaches the contact portion 11a. The current path at this time is the arc electrode 11.
When viewed from above, it looks as shown by the solid line in Figure G4, and a magnetic field parallel to the arc is generated on the entrance surface of the arc electrode 11 in four regions. If an arc 14 is generated at the contact portion 11a, as shown in FIG. 4, it spreads from the center 1, where the magnetic field is very weak, to the center 1, where the magnetic field is strong, and is extinguished there.

平行磁界形成極の特徴は前述した如く、アーク電極構造
にひろけて局部的な溶融を防ぎ、しゃ断性能を向トする
ことにあるが、このような電極でも、電極材料によって
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、つ1」えばC11−P l:1合金
やCu−B1舎金などを用いれば、これらは導電率や熱
伝導率が高いので通電性能にはすぐれているが、低融点
材Hのため、アークによって電極表面が溶け、多量の金
属蒸気を発生してしゃ断性能が悪い。寸だ、材料をCu
p e + Cu  Q r 、 CU  Q oなど
の合金にした場合、これらの(」利は面jアーク、11
σ1電圧1(1能にすぐれているため4. OK Aや
6:ロ(Aといった大電流をしや1祈り能であるが、前
述の合金に比らべ導′市率が低く、熱伝導率も約25%
イ4.1度に11(下するため、アーク電極11の11
fi電部] 1 c 、 1.1 (1の発熱が大きく
なり、定格電流や短時間電流の大きな・機種では、温度
十y1が試験規棺lll′I−を満足しなかったり、溶
着現象が発生したりする。従って、導電率、熱伝導率が
Cu −P I)合金と同等で、耐アーク性能がCL、
I −1・゛e0舎金同じJ:うな旧利があれば問題な
く40KA級や63K A級の真空バルブを作ることが
出来る。しか17、実際には両方を満足する(」刺はな
く、そのため、第5図の如きアーク電極20の構造にし
て、通電とし−や1仇の両性能全満足させる真空バルブ
としていた。第5図のアーク電極20に12、耐アーク
、面1電圧性能のよいCu−Fe合金等の4」料を使月
1した表向電極21と導電率、熱伝導率のよいC1lな
どを使用した裏面アーク市極部22とを接合したもので
、このようなアーク電極構造にすると、11111アー
ク、面1電圧性能は表面アーク市極部21で、また、通
電、短時間性能は表向アーク電極部22で受は持つこと
になり、通電としゃ断の両性能を満足させることができ
る。
As mentioned above, the feature of the parallel magnetic field forming pole is that it spreads over the arc electrode structure to prevent local melting and improve the breaking performance, but even with such electrodes, the performance is affected by the electrode material. is inevitable. In other words, if a material such as C11-Pl:1 alloy or Cu-B1 metal is used as the material for the arc electrode 11, these materials have high electrical conductivity and thermal conductivity, so they have excellent current carrying performance. Since the material H is a low-melting point material, the electrode surface is melted by the arc, generating a large amount of metal vapor, resulting in poor interrupting performance. The material is Cu.
When alloyed with p e + Cu Q r, CU Q o, etc., these (') are plane j arc, 11
σ1 Voltage 1 (1) Because it is excellent in 4. OK A and 6: B (A), it can handle large currents and has 1 prayer ability, but its conductivity is lower than the above-mentioned alloys, and it has poor thermal conductivity. The rate is also about 25%
11 (to lower the arc electrode 11)
1c, 1.1 (For models with large rated currents and short-time currents, the heat generation of 1 becomes large, and the temperature 1y1 does not satisfy the test standard 11'I-, or the welding phenomenon occurs. Therefore, the electrical conductivity and thermal conductivity are equivalent to Cu-P I) alloys, and the arc resistance is CL,
I-1・゛e0Same money J: If you have the old profit, you can make a 40KA class or 63KA class vacuum valve without any problem. However, in reality, there was no problem in satisfying both of the requirements.Therefore, the structure of the arc electrode 20 as shown in Fig. 5 was used to create a vacuum valve that completely satisfied both the performance of energization and the first and second functions. The arc electrode 20 shown in the figure is made of 4" material such as Cu-Fe alloy, which has good arc resistance and surface voltage performance, and the back surface is made of material such as C1L, which has good electrical conductivity and thermal conductivity. With this type of arc electrode structure, the 11111 arc, surface 1 voltage performance is achieved by the surface arc electrode part 21, and the energization and short-time performance is determined by the surface arc electrode part. 22 has a receiver, and can satisfy both energizing and cutting off performance.

しかし、この電極構造にした場合、高価格で導電率の低
い表面アーク電極部21は出来るだけ薄くして、その反
対に、低価格で導電率の高い裏面アーク電極部22は相
対的に出来るだけ厚くした方が、大容敏真空バルブ用電
極の小形化および原価低減に有効となるが、一方では、
高電界になる電極の外周端部は耐電圧性能の低い裏面ア
ーク電極部22の外周端部が大部分を占め、耐電圧性能
が悪く、高電圧大電流しや所用電極には不向きとなる欠
点がある。
However, in this electrode structure, the front arc electrode part 21, which is expensive and has low conductivity, is made as thin as possible, and on the contrary, the back arc electrode part 22, which is low cost and has high conductivity, is made as thin as possible. Thicker electrodes are more effective in reducing the size and cost of electrodes for large-capacity vacuum valves, but on the other hand,
The outer circumferential edge of the electrode where a high electric field is generated is mostly occupied by the outer circumferential edge of the back arc electrode part 22 which has low withstand voltage performance, and has a disadvantage that the withstand voltage performance is poor and it is unsuitable for use as an electrode for high voltage and large current applications. There is.

本発明の目的は前述の欠点を除き、通電性能、しゃ断性
能および耐電圧性能ともすぐれた電極にし、12KV級
以上の電圧で、25 K A以−七の大電流を通電し、
しゃ断する真空バルブを提供することにある。
The purpose of the present invention is to eliminate the above-mentioned drawbacks, to create an electrode with excellent current carrying performance, breaking performance, and withstand voltage performance, to conduct a large current of 25 K A or more at a voltage of 12 KV class or higher, and to
The purpose is to provide a vacuum valve that shuts off the vacuum.

本発明は、裏面アーク電極部及びコイル電極の外周端部
の表面にFe、cr、co等のT、N e族元素を接合
して、IIU1圧性能全性能させ、高電圧、大電流しゃ
所用電極としたものである。
In the present invention, T and Ne group elements such as Fe, Cr, and Co are bonded to the surface of the back arc electrode part and the outer peripheral end of the coil electrode to achieve full IIU 1-voltage performance, and for high voltage and large current shielding applications. It is used as an electrode.

第6図は本発明からなる電極3oで、表面アーク電極部
31、裏面アーク電極部32、コイル電極33、ホルダ
ー34、裏面アークg極部32とコイル電極33の外周
端部を覆う面j電圧すング層部35より構造されでいる
。表面アーク電・険31は耐アーク、耐電圧性能はよい
が、導電率、熱電率の低いCu −F’ e 、 Cu
 −Cr 、 cll−coなどの合金材料である。裏
面アーク電極32及びコイル電極33は導電率、熱電率
の高いC11などを使用する。寸だ、耐tE圧リング層
部35は1″e。
FIG. 6 shows the electrode 3o according to the present invention, and the surface j voltage covering the front arc electrode part 31, the back arc electrode part 32, the coil electrode 33, the holder 34, the back arc g pole part 32, and the outer peripheral end of the coil electrode 33. The ring layer portion 35 is structured as follows. Surface arc electric resistance 31 has good arc resistance and withstand voltage performance, but has low electrical conductivity and thermal conductivity.
-Alloy materials such as Cr and cll-co. The back arc electrode 32 and the coil electrode 33 are made of C11 or the like, which has high electrical conductivity and high thermoelectric coefficient. The tE pressure ring layer portion 35 is 1″e.

Cr、CO等のドc族元素をメッキ」たd、スパッタリ
ングなどの方法で裏面アーク屯極部32とコイル電極3
3の外周端部の表面を覆って接合されたものである。
The back arc electrode part 32 and the coil electrode 3 are coated with C-group elements such as Cr and CO by a method such as plating or sputtering.
It is joined to cover the surface of the outer peripheral end of No. 3.

本電極30の構造にすると、定格電流および定格しゃ断
電流の大きな機種で、導′i11率や熱電率のよいQu
を表向アーク電、j血32に使用しているため、アーク
電極の発生熱量が低く押えられ、熱伝導もCLI−pe
金合金の約4倍高くなるので、通電性能および短時間電
流性能がよい。
With the structure of this electrode 30, Qu
Since CLI-pe is used for the surface arc electrode, the amount of heat generated by the arc electrode is kept low, and the heat conduction is also better than that of CLI-pe.
Since it is about 4 times more expensive than gold alloy, it has good current carrying performance and short-time current performance.

一方、大電流しや]析時には、第4図で説明した如く、
アーク電極の主接触部11aに発生したアーク14はm
lアーク性のよいCu −1’i” e合金などの材料
を使用しでいる表面アーク醒極部31にひろがり、消弧
される。消弧直後、電極間に印加される苛酷な再起電圧
や開極中の電極間に印加されるインパルス電圧などは、
高電界になる電極の外周端部の表面が耐電圧性能のよい
p e族元素で覆われているので、七分、耐えることが
できる。
On the other hand, when analyzing a large current, as explained in Fig. 4,
The arc 14 generated at the main contact part 11a of the arc electrode is m
The arc spreads to the surface arc extinguishing section 31, which is made of a material such as a Cu-1'i'' alloy with good arcing properties, and is extinguished. Immediately after the arc is extinguished, severe re-energization voltage and The impulse voltage applied between the electrodes during opening, etc.
Since the surface of the outer peripheral edge of the electrode, which is subject to high electric fields, is covered with a PE group element that has good withstand voltage performance, it can withstand up to 7 minutes.

第7図及び第8図は本発明の変形例で、lft電圧リン
グ層部35を、第7図は裏面アーク電極部32の外周端
部表面にのみ、実施したもの、また第8図は高電界にな
る裏面アーク電極部32とコイル電極33の外周端R部
表面のみ実施したもので、第6図の電極30と同一の効
果がある。
7 and 8 show modified examples of the present invention, in which the lft voltage ring layer 35 is formed only on the outer peripheral end surface of the back arc electrode section 32 in FIG. 7, and in FIG. This is carried out only on the surface of the outer peripheral end R portion of the back arc electrode portion 32 and the coil electrode 33, which generates an electric field, and has the same effect as the electrode 30 in FIG. 6.

本発明によれば、耐アーク性能および耐電圧性能のよい
材料を表面アーク電極部に、また導電率および熱伝導率
のよいC1,1を裏面アーク′11テ極部にして、裏面
アーク電+li部とコイル′]に極の外周端部の表向を
4電圧性能のよい’Ji’e族元素で覆っているので、
12KV級以上の高電圧で“、大電流通電およびしゃ断
の両性能にすぐ扛だ電極が安価に出来ると云う効果があ
る。
According to the present invention, a material with good arc resistance and withstand voltage performance is used for the front arc electrode part, and C1,1 with good electrical conductivity and thermal conductivity is used for the back arc '11 tip part, so that the back arc electrode +li Since the surface of the outer peripheral end of the pole is covered with a 'Ji'e group element with good 4-voltage performance,
At high voltages of 12KV class or higher, it has the advantage of being able to produce electrodes at low cost that can quickly perform both large current conduction and cutoff.

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

第1図は従来の真空バルブを示す縦断面図、第2図は従
来の電極を示す)915分1仇而図、第3図はその分解
図、第4図は磁界の状況説明図、第5図は第1図とは異
なる従来の電極を示す断面図、第6図(A)およびa′
3)は本発明の実施例を示す部分平向および断面図、第
7図及び第8図は本発明の異なる実施例の断面図である
。 30・・・電極、31・・・表面部、32・・・裏面部
、33・・・コイル電極、34・・・ホルダ、35・・
・耐電圧リン糖30 第5図 (A)    第60  (B)
Figure 1 is a vertical sectional view showing a conventional vacuum valve, Figure 2 is a 1:915 diagram showing a conventional electrode, Figure 3 is an exploded view, Figure 4 is a diagram explaining the state of the magnetic field, 5 is a sectional view showing a conventional electrode different from that in FIG. 1, and FIG. 6(A) and a'
3) is a partial plan view and a cross-sectional view showing an embodiment of the present invention, and FIGS. 7 and 8 are cross-sectional views of different embodiments of the present invention. 30... Electrode, 31... Surface portion, 32... Back surface portion, 33... Coil electrode, 34... Holder, 35...
・Withstand voltage phosphorus sugar 30 Figure 5 (A) Figure 60 (B)

Claims (1)

【特許請求の範囲】[Claims] 1、真空容器内に接離可能な少なくとも一対のアーク電
極を配置し、アーク電極裏面より真空容器外に延びるロ
ッドと、少なくとも一方のロッドとアーク電極との間に
電気的に接続し、かつアークに対して平行な磁界を発生
するコイル電極を有する真空しゃ断器において、上記ア
ーク電極はアークを点弧する表面部と、表向部の裏面に
表面部より電気伝導率の良い材料を使用することを特徴
とする真空しゃ断器用電極。
1. At least a pair of arc electrodes that can be brought into contact and separated from each other are arranged in a vacuum vessel, and a rod that extends outside the vacuum vessel from the back surface of the arc electrode is electrically connected between at least one rod and the arc electrode, and In a vacuum breaker having a coil electrode that generates a magnetic field parallel to the arc electrode, the arc electrode uses a material with higher electrical conductivity than the front surface for the front surface that ignites the arc and the back surface of the front surface. An electrode for vacuum breaker featuring the following.
JP16708081A 1981-10-21 1981-10-21 Electrode for vacuum breaker Pending JPS5868819A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16708081A JPS5868819A (en) 1981-10-21 1981-10-21 Electrode for vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16708081A JPS5868819A (en) 1981-10-21 1981-10-21 Electrode for vacuum breaker

Publications (1)

Publication Number Publication Date
JPS5868819A true JPS5868819A (en) 1983-04-23

Family

ID=15843024

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16708081A Pending JPS5868819A (en) 1981-10-21 1981-10-21 Electrode for vacuum breaker

Country Status (1)

Country Link
JP (1) JPS5868819A (en)

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