JPH0777101B2 - Contact for vacuum switch - Google Patents

Contact for vacuum switch

Info

Publication number
JPH0777101B2
JPH0777101B2 JP10158487A JP10158487A JPH0777101B2 JP H0777101 B2 JPH0777101 B2 JP H0777101B2 JP 10158487 A JP10158487 A JP 10158487A JP 10158487 A JP10158487 A JP 10158487A JP H0777101 B2 JPH0777101 B2 JP H0777101B2
Authority
JP
Japan
Prior art keywords
alloy
vapor pressure
contact
region
arc
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.)
Expired - Lifetime
Application number
JP10158487A
Other languages
Japanese (ja)
Other versions
JPS63266720A (en
Inventor
功 奥富
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 JP10158487A priority Critical patent/JPH0777101B2/en
Publication of JPS63266720A publication Critical patent/JPS63266720A/en
Publication of JPH0777101B2 publication Critical patent/JPH0777101B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H33/00High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
    • H01H33/60Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
    • H01H33/66Vacuum switches
    • H01H33/664Contacts; Arc-extinguishing means, e.g. arcing rings
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H33/00High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
    • H01H33/60Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
    • H01H33/66Vacuum switches
    • H01H33/664Contacts; Arc-extinguishing means, e.g. arcing rings
    • H01H33/6644Contacts; Arc-extinguishing means, e.g. arcing rings having coil-like electrical connections between contact rod and the proper contact

Landscapes

  • Contacts (AREA)
  • High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、真空開閉器における真空バルブ用接点に関す
る。
DETAILED DESCRIPTION OF THE INVENTION Object of the Invention (Field of Industrial Application) The present invention relates to a contact for a vacuum valve in a vacuum switch.

(従来の技術) 真空開閉器は、他の開閉器に比較し、小型、軽量、メン
テナンスフリー、環境調和等種々の優れた特徴を有する
ため、近年次第にその適用範囲が拡大されてきた。真空
しゃ断器は、真空中でのアーク拡散性を利用して高真空
中で電流しゃ断を行なうものであり、その側断面を示し
た第4図を参照し説明する。
(Prior Art) Since the vacuum switch has various excellent features such as small size, light weight, maintenance-free and environmental harmony as compared with other switches, its application range has been gradually expanded in recent years. The vacuum circuit breaker utilizes the arc diffusivity in a vacuum to perform current cutting in a high vacuum, and will be described with reference to FIG. 4 showing a side cross section thereof.

真空しゃ断器は真空気密に保たれたしゃ断室1を有し、
これは絶縁材料によりほぼ円筒状に形成された絶縁容器
2と、この両端に封止金具3a,3bを介して設けた金属製
の蓋体4a,4bとで構成されている。
The vacuum breaker has a breaking chamber 1 that is kept vacuum-tight,
This is composed of an insulating container 2 formed of an insulating material in a substantially cylindrical shape, and metallic lids 4a and 4b provided on both ends of the insulating container 2 via sealing metal fittings 3a and 3b.

しゃ断室1内には、導電棒5,6の対向する端部に取付け
られた一対の固定電極7、可動電極8が配設される。可
動電極8の導電棒6にはベローズ9が取付けられ、しゃ
断室1内の真空気密を保持しつつ可動電極8が軸方向に
移動する。ベローズ9の上部には金属製のアークシール
ド10が設けられ、ベローズ9がアーク蒸気で覆われるこ
とを防止している。同様に金属製のアークシールド11
は、しゃ断室1内において固定電極7および可動電極8
を覆うように設けられ、絶縁容器2がアーク蒸気で覆わ
れることを防止している。通電中は固定接点13bに可動
接点13aが接触しており、電流のしゃ断は同導電棒を下
方向へ移動させ、この両接点の接触を断つことにより行
なう。
A pair of fixed electrodes 7 and movable electrodes 8 attached to opposite ends of the conductive rods 5 and 6 are arranged in the interrupting chamber 1. A bellows 9 is attached to the conductive rod 6 of the movable electrode 8 so that the movable electrode 8 moves in the axial direction while maintaining vacuum tightness in the blocking chamber 1. A metal arc shield 10 is provided above the bellows 9 to prevent the bellows 9 from being covered with arc vapor. Similarly metal arc shield 11
Is a fixed electrode 7 and a movable electrode 8 in the shutoff chamber 1.
To prevent the insulating container 2 from being covered with arc vapor. The movable contact 13a is in contact with the fixed contact 13b during energization, and the current is cut off by moving the conductive rod downward and breaking the contact between these two contacts.

次に、導電棒5,6と電極7,8、電極7,8と接点13a,13bとの
相互の固定構造について、第4図における可動電極8周
辺の詳細を示した第5図を参照し説明する。可動電極8
は導電棒6に符号12で示されたろう付または図示しない
かしめ等により固定され、可動接点13aは可動電極8に
符号14で示されたろう付または図示しないかしめ等によ
り固定される。固定側の固定電極7と接点13bとの固定
方法も同様である。
Next, with respect to the mutual fixing structure of the conductive rods 5 and 6 and the electrodes 7 and 8 and between the electrodes 7 and 8 and the contacts 13a and 13b, refer to FIG. 5 showing the details around the movable electrode 8 in FIG. explain. Movable electrode 8
Is fixed to the conductive rod 6 by brazing indicated by reference numeral 12 or caulking not shown, and the movable contact 13a is fixed at the movable electrode 8 by brazing indicated by reference numeral 14 or caulking not shown. The same applies to the method of fixing the fixed electrode 7 and the contact 13b on the fixed side.

(発明が解決しようとする問題点) 真空開閉器用接点に要求される要件として、(1)溶着
性が少ないこと、(2)耐電圧が高いこと、(3)耐消
耗性に優れること、(4)接触抵抗が低く安定している
こと、等がある。この他に最近の真空開閉装置に対する
期待が一層高まり、(5)低サージ機能を有すること、
(6)大電流しゃ断機能を有することが要求されるが、
この二つの要求は相反するものである。
(Problems to be Solved by the Invention) Requirements for a contact for a vacuum switch are: (1) low weldability, (2) high withstand voltage, (3) excellent wear resistance, 4) The contact resistance is low and stable. In addition to this, expectations for recent vacuum switchgear have further increased, and (5) it has a low surge function,
(6) It is required to have a large current cutoff function,
These two requirements are in conflict.

まず、低サージ機能を有するための要件について説明す
る。電動機負荷等の誘導回路で電流をしゃ断する時など
において、過度のサージ電圧を発生させ、負荷機器の絶
縁を破壊させる恐れがある。この異常サージ電圧の発生
原因は、真空中におけるしゃ断時に低電流側に発生する
電流さい断現象(交流電流波形の自然ゼロ点を待たずに
強制的に電流しゃ断が行なわれること。)によるもので
ある。異常サージ電圧の値VSは回路のサージインピーダ
ンスZOと電流さい断値ICの積、すなわちVS=2ZO・IC
表わされ、異常サージ電圧VSを低くするためには、つま
り低サージ機能を有するためには、電流さい断値ICを小
さくしなければならない。従って、しゃ断時において、
アークによって可動接点13aと固定接点13bの各表面から
イオン、金属粒子が多く蒸発して両接点間に浮遊し、ア
ークが容易に接続されなければならない。従って、接点
13a,13bに用いられる材料は、大電流をしゃ断する時の
みならず、開閉電流が小さくて接点の温度上昇が小さい
場合であっても蒸発性の高い高蒸気圧性を有することが
要求される。
First, the requirements for having a low surge function will be described. When the current is cut off by an induction circuit such as a motor load, an excessive surge voltage may be generated, and the insulation of the load device may be destroyed. The cause of this abnormal surge voltage is due to the current interruption phenomenon that occurs on the low current side during interruption in vacuum (forced current interruption without waiting for the natural zero point of the AC current waveform). is there. The value of the abnormal surge voltage V S is represented by the product of the surge impedance Z O of the circuit and the current interruption value I C , that is, V S = 2Z O · I C , and in order to lower the abnormal surge voltage V S , That is, in order to have a low surge function, the current threshold value I C must be reduced. Therefore, at the time of interruption,
A large amount of ions and metal particles evaporate from each surface of the movable contact 13a and the fixed contact 13b by the arc and float between the contacts, so that the arc must be easily connected. Therefore, the contact
The materials used for 13a and 13b are required to have high vapor pressure, which is highly vaporizable, not only when blocking a large current, but also when the switching current is small and the temperature rise of the contact is small.

このような低サージ機能を満たすものとして、高蒸気圧
性材料であるAgを含有したAg-WC合金が知られている。
この合金から成る接点は、 (1) WCの介在が接点表面からのイオンの放射を容易
にさせること、 (2) 電界放射電子の衝突による電極面の加熱に基づ
く接点表面から金属粒子の蒸発を促進させること、 (3) 接点材料中の炭化物がアークにより分解し、荷
電体を生成すること、等により、優れた低サージ機能を
有している。この他にこの機能を有する材料として、高
蒸気圧性材料であるCuを含有したCu-Cr合金、Cu-Bi合金
等が知られている。
As a material satisfying such a low surge function, an Ag-WC alloy containing Ag, which is a high vapor pressure material, is known.
The contacts made of this alloy have (1) the interposition of WC facilitates the emission of ions from the contact surface, and (2) the evaporation of metal particles from the contact surface due to the heating of the electrode surface due to the collision of field emission electrons. It has an excellent low surge function by accelerating, (3) Carbide in the contact material is decomposed by an arc to generate a charged body, and the like. In addition to this, as a material having this function, a Cu-Cr alloy containing Cu, which is a high vapor pressure material, a Cu-Bi alloy, and the like are known.

これに対し、もう一方の相反する要件である大電流しゃ
断機能を有するためには接点が低蒸気圧性の材料から成
ることが要求される。大電流をしゃ断する場合には接点
の表面温度は極めて高温となるが、このような場合であ
ってもアークによる接点表面からの蒸発量が少なく、両
接点間にイオン、金属粒子がほとんど浮遊しない状態で
なければしゃ断性が損われることとなる。従って一般に
どちらか一方の機能の向上を追及すると、もう一方の機
能が低下する。
On the other hand, the contacts are required to be made of a material having a low vapor pressure in order to have the large current interruption function which is the other contradictory requirement. When shutting off a large current, the contact surface temperature becomes extremely high, but even in such a case, the amount of evaporation from the contact surface due to the arc is small, and ions and metal particles hardly float between both contacts. If it is not in a state, the cutoff property will be impaired. Therefore, in general, when one of the functions is improved, the other function is deteriorated.

この二つの相反する要件を満たすための手段として、接
点を高蒸気圧性材料と低蒸気圧性材料の二種類の材料か
ら構成するものがある。電流をしゃ断するために通電中
接触していた両接点が離れる際において、初めに高蒸気
圧性材料から成る部分から多くのイオン、金属粒子が蒸
発して接点間に浮遊し、アークがこれに導かれて両接点
における高蒸気圧性材料同志に接続される。低サージ機
能が満たされるために必要な時間経過後両接点における
高蒸気圧性材料同志に接続されていたアークを両接点に
おける低蒸気圧性材料同志に接続されるように、アーク
を移行させる。これは、第7図に示されたコイル電極4
4、第8図に示されたスパイラル電極45等を用いて縦磁
界Hを制御することにより両接点間に浮遊するイオン、
金属粒子の分布を変えて強制的にアークを移行させると
いう方法等により行なうことができる。
As a means for satisfying these two conflicting requirements, there is one in which the contact is made of two kinds of materials, a high vapor pressure material and a low vapor pressure material. When the contacts that were in contact during energization to separate the current are separated from each other, many ions and metal particles evaporate from the part made of the material with high vapor pressure and float between the contacts, and the arc guides them. It is connected to the high vapor pressure material comrades at both contacts. After a lapse of time necessary for satisfying the low surge function, the arc is moved so that the arc, which was connected to the high vapor pressure material at both contacts, is connected to the low vapor pressure material at both contacts. This is the coil electrode 4 shown in FIG.
4, Ions floating between both contacts by controlling the longitudinal magnetic field H using the spiral electrode 45 shown in FIG.
This can be performed by changing the distribution of the metal particles and forcibly moving the arc.

しかし、低電流しゃ断時にも低サージ機能を有する高蒸
気圧性材料の物性と、大電流しゃ断機能を有する低蒸気
圧性材料の物性とでは蒸気圧性という点において大きく
異なる。このため、縦磁界により両接点間に浮遊するイ
オン、金属粒子の分布を変えても、アークが高蒸気圧性
材料から成る部分と低蒸気圧性材料から成る部分との境
界上に停滞し、容易に移行しない。従って、接点を高蒸
気圧性材料と低蒸気圧性材料とを単純に組み合せて構成
しただけでは低サージ機能と大電流しゃ断機能とを同時
に満たすことはできない。
However, the physical properties of a high vapor pressure material having a low surge function even at low current interruption and the physical properties of a low vapor pressure material having a large current interruption function differ greatly in terms of vapor pressure characteristics. Therefore, even if the distribution of ions and metal particles floating between both contacts is changed by the longitudinal magnetic field, the arc stagnates on the boundary between the part made of high vapor pressure material and the part made of low vapor pressure material, and it is easy to Do not move. Therefore, the low surge function and the large current cutoff function cannot be satisfied at the same time by simply configuring the contact point by simply combining the high vapor pressure material and the low vapor pressure material.

上述した事情に鑑み、電流しゃ断時における高蒸気圧性
材料から低蒸気圧性材料へのアークの移行が停滞せずに
容易に行なわれ、低サージ機能と大電流しゃ断機能とい
う二つの相反する機能を有した真空開閉器用接点を提供
することを目的とする。
In view of the above-mentioned circumstances, the arc transfer from the high vapor pressure material to the low vapor pressure material at the time of current interruption is easily performed without stagnation, and it has two contradictory functions of low surge function and large current interruption function. An object of the present invention is to provide a contact for a vacuum switch.

〔発明の構成〕[Structure of Invention]

(問題点を解決するための手段) 本発明の真空開閉器用接点は、2種類の合金領域とその
間にはさまれた境界領域が同心円状に配され、前記合金
領域の各々が蒸気圧の高さの異なる材料から成り、前記
境界領域が半径方向に蒸気圧の高さが連続して異なるよ
うに組成された材料から成ることを特徴としている。
(Means for Solving the Problems) In the vacuum switch contact of the present invention, two alloy regions and a boundary region sandwiched therebetween are concentrically arranged, and each of the alloy regions has a high vapor pressure. It is characterized in that the boundary region is made of a material having different vapor pressure levels continuously in the radial direction.

(作用) 本発明の真空開閉器用接点において、外周側に位置した
合金領域が内周側に位置した合金領域よりも蒸気圧が高
い材料で構成されている場合には、境界領域(B1)を構
成する材料の蒸気圧の高さは半径方向に対して外周側か
ら内周側へ向かうに従って連続領域に低くなる。このた
め、材料の蒸気圧の高さは合金領域(A1)から境界領域
(B1)を経て合金領域(A2)へ向かうに従って徐々に低
くなることになる。このような真空開閉器用接点を真空
開閉器に用いて電流しゃ断を行なう場合、通電中に接触
していた両接点が離れる際に、接点を構成している領域
のうち最も蒸気圧の高い材料から成る外周側に位置した
合金領域から多くのイオン、金属粒子が蒸発して両接点
のこの合金領域同志の間に浮遊し、アークがこれに導か
れて両者の間に接続される。
(Operation) In the vacuum switch contact of the present invention, when the alloy region located on the outer peripheral side is made of a material having a higher vapor pressure than the alloy region located on the inner peripheral side, the boundary region (B 1 ) The height of the vapor pressure of the material forming the element decreases in the continuous region from the outer peripheral side toward the inner peripheral side in the radial direction. Therefore, the height of the vapor pressure of the material gradually decreases from the alloy region (A 1 ) to the boundary region (B 1 ) to the alloy region (A 2 ). When current is cut off using such a vacuum switch contact for a vacuum switch, when the two contacts that were in contact with each other during energization are separated, the material with the highest vapor pressure in the region that makes up the contact is selected. Many ions and metal particles evaporate from the alloy region located on the outer peripheral side and float between the alloy regions of both contact points, and an arc is guided to this and connected between the two.

この後、縦磁界の制御により両接点間に浮遊するイオ
ン、金属粒子の分布を変えると、外周側に位置した合金
領域から境界領域へアークが向かう。材料の蒸気圧の高
さは、外周側の合金領域から境界領域を経て内周側の合
金領域へ向かうに従って徐々に低くなるため、アークは
停滞することなく容易に境界領域へ移行する。このよう
にして縦磁界の制御により、強制的にアークを内周側の
合金領域へ向かって移行させていく。そして低サージ機
能が満たされるためにつまりアークが両接点間に接続さ
れているために必要な時間経過後、最も蒸気圧が低くほ
とんどアーク、金属粒子が蒸発しない内周側の合金領域
へ移行させると、この瞬間にアークの接続が断たれるこ
ととなる。
After that, when the distribution of ions and metal particles floating between both contacts is changed by controlling the longitudinal magnetic field, the arc is directed from the alloy region located on the outer peripheral side to the boundary region. The height of the vapor pressure of the material gradually decreases from the alloy region on the outer peripheral side to the alloy region on the inner peripheral side through the boundary region to the alloy region on the inner peripheral side, so that the arc easily transitions to the boundary region without stagnation. In this way, by controlling the longitudinal magnetic field, the arc is forcibly moved toward the alloy region on the inner peripheral side. Then, after the time required for satisfying the low surge function, that is, because the arc is connected between both contacts, the vapor pressure is the lowest and the arc moves to the inner alloy region where metal particles do not evaporate. Then, at this moment, the arc connection will be cut off.

この場合とは逆に、内周側に位置した合金領域の方が外
周側に位置した合金領域よりも蒸気圧が高い材料で構成
されている場合には、境界領域の材料の蒸気圧の高さは
半径方向に対して内周側から外周側へ向かうに従って連
続的に低くなる。このため、材料の蒸気圧の高さは内周
側の合金領域から境界領域を経て外周側の合金領域へ向
かうに従って徐々に低くなることになる。この場合に
は、まずアークは両接点における内周側の合金領域の間
に接続され、縦磁界の制御により境界領域を経て外周側
の合金領域へ向かってアークが移行し、アークの接続が
断たれる。
On the contrary, when the alloy region located on the inner peripheral side is composed of a material having a higher vapor pressure than the alloy region located on the outer peripheral side, the vapor pressure of the material in the boundary region is high. The depth decreases continuously from the inner circumference side to the outer circumference side in the radial direction. For this reason, the vapor pressure of the material gradually decreases from the alloy region on the inner peripheral side to the alloy region on the outer peripheral side via the boundary region. In this case, the arc is first connected between the alloy areas on the inner circumference side of both contacts, and the arc is transferred to the alloy area on the outer circumference side through the boundary area by the control of the longitudinal magnetic field, and the arc is disconnected. Be drunk

(実施例) 本発明の一実施例として、接点が2種類の合金領域
(A1)および(A2)と境界領域(B1)からなる場合につ
いて、接点を上部から見た第1図を用いて説明する。第
6図に示した従来の接点と比較し、合金領域(A1)21と
合金領域(A2)23との間に中間領域(B1)22が配されて
いる点が異なる。合金領域(A1)21と合金領域(A2)23
とは、それぞれ含有量の異なる同一の合金系材料からな
る場合と、異なる合金系材料からなる場合がある。中間
領域(B1)22の合金系材料は、合金領域(A1)21と合金
領域(A2)23のいずれとも異なる場合、または少なくと
もどちらか一方の合金系材料と同一で含有量が異なる場
合がある。
(Example) As an example of the present invention, FIG. 1 is a top view of the contact in the case where the contact is composed of two kinds of alloy regions (A 1 ) and (A 2 ) and a boundary region (B 1 ). It demonstrates using. It differs from the conventional contact shown in FIG. 6 in that an intermediate region (B 1 ) 22 is arranged between the alloy region (A 1 ) 21 and the alloy region (A 2 ) 23. Alloy area (A 1 ) 21 and alloy area (A 2 ) 23
And may be made of the same alloy-based material having different contents, or may be made of different alloy-based materials. The alloy-based material of the intermediate area (B 1 ) 22 is different from both the alloy area (A 1 ) 21 and the alloy area (A 2 ) 23, or at least one of the alloy-based materials has a different content. There are cases.

合金領域(A1)21と合金領域(A2)23との合金系材料が
同一の場合、例えばAg-WC系合金の場合には、どちらか
一方の領域には低サージ機能を有する材料として蒸気圧
の高い金属であるAgの含有量の多い40Ag-WC-10Co(数値
は重量%を示すものとする。以下同様)を用い、もう一
方の合金領域には大電流しゃ断機能を有する材料として
Agの含有量の少ない30Ag-WC-0.2Coを用いることができ
る。この場合の境界領域には、両方の合金領域に用いら
れる合金系つまりAg-WC系合金と異なる合金系を用いる
場合と、同一の合金系であるAg-WC系合金を用いる場合
があり、いずれにおいても材料の組成が半径方向に対し
て連続して異なる分布となっており、これにより材料の
蒸気圧の高さが半径方向に対し連続して異なる。
If the alloy region (A 1 ) 21 and the alloy region (A 2 ) 23 are made of the same alloy material, for example, Ag-WC alloy, one of the regions has a low surge function. 40Ag-WC-10Co (numerical value shows% by weight; the same applies hereinafter) with a high content of Ag, which is a metal with a high vapor pressure, was used as a material with a large current interruption function in the other alloy region.
30Ag-WC-0.2Co with a low Ag content can be used. In the boundary region in this case, there are cases where an alloy system used for both alloy regions, that is, an alloy system different from the Ag-WC system alloy, and a case where the same alloy system Ag-WC system alloy is used. Also in the above, the composition of the material has a distribution that continuously differs in the radial direction, and thus the height of the vapor pressure of the material continuously differs in the radial direction.

合金領域(A1)21と合金領域(A2)23は、いずれか一方
が高蒸気圧性材料からなり、もう一方が低蒸気圧性材料
からなるが、合金領域(A1)21が高蒸気圧性材料からな
る場合には、中間領域(B1)22の材料の蒸気圧の高さの
値を占める範囲は、合金領域(A1)21の蒸気圧の高さの
値と合金領域(A2)23の蒸気圧の高さの値との間にあ
り、さらに材料の蒸気圧の高さの半径方向に対する分布
が外周側から内周側へ向かって連続して低くなる。合金
領域(A1)21が低蒸気圧性材料からなる場合にはこの逆
であり、合金領域(A2)23が高蒸気圧性材料からなり、
中間領域(B1)22の蒸気圧の高さの値の占める範囲は、
合金領域(A1)21の蒸気圧の高さの値と合金領域(A2
23の蒸気圧の高さの値との間にあり、さらに材料の蒸気
圧の高さの半径方向に対する分布は外周側から内周側へ
向かって連続して高くなる。この二通りのいずれの組合
せも可能である。以下に合金領域(A2)23が高蒸気圧性
材料からなる場合について説明する。
One of the alloy area (A 1 ) 21 and the alloy area (A 2 ) 23 is made of a high vapor pressure material and the other is made of a low vapor pressure material, but the alloy area (A 1 ) 21 is made of a high vapor pressure material. When the material is made of a material, the range of the vapor pressure height value of the material in the intermediate region (B 1 ) 22 is determined by the vapor pressure height value of the alloy region (A 1 ) 21 and the alloy region (A 2 ) 23 of the vapor pressure height value, and the distribution of the vapor pressure height of the material in the radial direction continuously decreases from the outer peripheral side to the inner peripheral side. The opposite is true when the alloy area (A 1 ) 21 consists of a low vapor pressure material, and the alloy area (A 2 ) 23 consists of a high vapor pressure material,
The range occupied by the high vapor pressure value in the intermediate region (B 1 ) 22 is
Value of vapor pressure height of alloy area (A 1 ) 21 and alloy area (A 2 )
23 and the vapor pressure height value of 23, and the distribution of the vapor pressure height of the material in the radial direction continuously increases from the outer peripheral side to the inner peripheral side. Any combination of these two ways is possible. The case where the alloy region (A 2 ) 23 is made of a high vapor pressure material will be described below.

まず、このような組成を有する接点を製造する方法の一
例を示す。成型金型として、第2図に示した金型31、第
1のポンチ32、第2のポンチ35、金型台37を用いる。
First, an example of a method of manufacturing a contact having such a composition will be shown. As the molding die, the die 31, the first punch 32, the second punch 35, and the die stand 37 shown in FIG. 2 are used.

第1のポンチ32を金型31から取りはずし、第2のポンチ
35をその底部35aが金型台37に接触した状態となるよう
に設置する。金型31と第2のポンチ35との空間に合金領
域(A1)21を形成するための粉末を混合調製して充填
し、第1のポンチ32により成型圧力P1で加圧する。次に
第2のポンチ35を一旦金型31から抜き出し、その空間38
に合金領域(A2)23を形成するための粉末を混合調製し
て充填し、第2のポンチ35により成型圧力P2で加圧す
る。この場合の圧力P2は、合金領域(A1)21と合金領域
(A2)23に同一の合金系を用いた場合には、合金領域
(A2)23に後に多くのAgを溶浸させるよう、P1よりも小
さくして、空孔の占める割合を多くする。合金領域
(A1)21と合金領域(A2)23に異なる合金系を用いる場
合には、圧力P2はP1と同一であってもよい。この場合の
境界領域(B1)22は、合金領域(A1)21と同一の粉末を
混合調製したものからなり、第1のポンチ32が有するテ
ーパ部32bにより加圧される圧力が半径方向に対して異
なり、合金領域(A1)21に近い外周側から合金領域
(A2)23に近い内周側へ近づくに従って低くなるため、
空孔の示す割合が多くなる。
Remove the first punch 32 from the mold 31 and remove the second punch
35 is installed so that its bottom portion 35a is in contact with the die stand 37. Powder for forming the alloy region (A 1 ) 21 is mixed and prepared in the space between the die 31 and the second punch 35, and the mixture is pressed by the first punch 32 at the molding pressure P 1 . Next, the second punch 35 is once pulled out of the mold 31, and the space 38
Powder for forming the alloy region (A 2 ) 23 is mixed and prepared and filled in, and is pressed with the molding pressure P 2 by the second punch 35. In this case, when the same alloy system is used in the alloy area (A 1 ) 21 and the alloy area (A 2 ) 23, the pressure P 2 is infiltrated with a large amount of Ag afterwards in the alloy area (A 2 ) 23. In order to make it so, it is made smaller than P 1 to increase the proportion of vacancy. When different alloy systems are used for the alloy area (A 1 ) 21 and the alloy area (A 2 ) 23, the pressure P 2 may be the same as P 1 . The boundary region (B 1 ) 22 in this case is made by mixing and preparing the same powder as the alloy region (A 1 ) 21, and the pressure applied by the tapered portion 32b of the first punch 32 is in the radial direction. However, unlike the alloy region (A 1 ) 21 from the outer peripheral side closer to the alloy region (A 2 ) 23 to the inner peripheral side, it becomes lower,
The proportion of holes is increased.

このようにして得られたものを円板状に形状を整える
と、第3図において中心軸方向の断面を示した成型体39
を得る。さらにこの成型体39を非酸化性雰囲気中で焼結
するとスケルトンを得る。このスケルトンの一方の面に
AgまたはCuなどの高蒸気圧性材料を接触させ、非酸化性
雰囲気中でこれらの融点以上の温度でスケルトンを加熱
し、スケルトンの有する空孔中にAgまたはCuなどを溶浸
させる。この方法により、一定の組成を持ち低蒸気圧性
材料からなる合金領域(A1)21と、一定の組成を持ち高
蒸気圧性材料からなる合金領域(A2)23と、半径方向に
対してAgまたはCuの含有量の分布が異なり、外周側から
内周側へ向かうに従い含有量が多くなる。つまり内周側
へ向かうとともに蒸気圧が高くなる分布を有する材料か
らなる境界領域(B1)22を有した接点を得る。
When the thus obtained product is shaped into a disc, a molded body 39 showing a cross section in the direction of the central axis in FIG.
To get Further, if this molded body 39 is sintered in a non-oxidizing atmosphere, a skeleton is obtained. On one side of this skeleton
A high vapor pressure material such as Ag or Cu is brought into contact, the skeleton is heated at a temperature equal to or higher than these melting points in a non-oxidizing atmosphere, and Ag or Cu is infiltrated into the pores of the skeleton. According to this method, an alloy region (A 1 ) 21 made of a low vapor pressure material having a constant composition, an alloy region (A 2 ) 23 made of a high vapor pressure material having a constant composition, and Ag in the radial direction were used. Alternatively, the Cu content distribution is different, and the Cu content increases from the outer peripheral side toward the inner peripheral side. That is, a contact having a boundary region (B 1 ) 22 made of a material having a distribution in which the vapor pressure increases toward the inner peripheral side is obtained.

このようにして得られた接点を第7図に示すコイル電極
または第8図に示すスパイラル電極を有し、縦磁界の制
御を行なうことのできる第4図に示された真空開閉装置
の可動接点13aおよび固定接点13bに用いて電流しゃ断を
行なう場合について説明する。通電中接触していた両接
点13a,13bが離れる際に、両接点13a,13bを構成している
各合金領域のうち、最も高い蒸気圧材料からなる合金領
域(A2)23から多くのイオン、金属粒子が蒸発して両接
点間に浮遊し、アークがこれに導かれて両接点上の合金
領域(A2)23間に接続される。
The contact thus obtained has the coil electrode shown in FIG. 7 or the spiral electrode shown in FIG. 8, and the movable contact of the vacuum switchgear shown in FIG. 4 capable of controlling the longitudinal magnetic field. A case of performing current interruption using the 13a and the fixed contact 13b will be described. When the contacts 13a, 13b, which were in contact with each other during energization, separate from each other, many ions from the alloy region (A 2 ) 23 made of the highest vapor pressure material among the alloy regions forming the contacts 13a, 13b , The metal particles evaporate and float between the contacts, and an arc is guided to connect the alloy regions (A 2 ) 23 on the contacts.

この後、縦磁界の制御により、両接点間に浮遊するイオ
ン、金属粒子の分布が変わり、合金領域(A2)23から外
周側に隣接した境界領域(B1)22へ向かってアークが移
行する。境界領域(B1)22の材料の蒸気圧の高さは半径
方向に対して異なる分布を有し、内周側の部分の蒸気圧
は合金領域(A2)23の材料の蒸気圧の高さよりやや低
く、外周側へ向かうに従って徐々に高くなり、この外周
側の部分における蒸気圧の高さより、外周側に隣接した
合金領域(A1)21の材料の蒸気圧の高さの方がやや高
い。このため、縦磁界の制御により合金領域(A2)23か
ら境界領域(B1)22へ向かったアークは、各領域の境界
に停滞することなく境界領域(B1)22を経て合金領域
(A1)21へ容易に移行する。ここで、低サージ機能が満
たされるために必要な時間が経過するまでの間、材料の
蒸気圧が高く両接点間に多くのイオン、金属粒子が浮遊
してアークが接続される合金領域または境界領域の間に
アークが接続されつつ移行するようにし、その後大電流
しゃ断機能を満たすべく最も蒸気圧が低くイオン、金属
粒子がほとんど蒸発しない材料から成る合金領域(A1
21へアークを移行させるとその瞬間に両接点間のアーク
の接続が断たれる。
After that, by controlling the longitudinal magnetic field, the distribution of ions and metal particles floating between both contacts changes, and the arc moves from the alloy area (A 2 ) 23 to the boundary area (B 1 ) 22 adjacent to the outer peripheral side. To do. The height of the vapor pressure of the material in the boundary region (B 1 ) 22 has different distributions in the radial direction, and the vapor pressure of the inner peripheral portion is high in the vapor pressure of the material in the alloy region (A 2 ) 23. Slightly lower than the outer peripheral side, the vapor pressure of the material in the alloy region (A 1 ) 21 adjacent to the outer peripheral side is slightly higher than the vapor pressure of the outer peripheral side. high. Therefore, the arc heading from the alloy area (A 2 ) 23 to the boundary area (B 1 ) 22 by controlling the longitudinal magnetic field does not stay at the boundary of each area and passes through the boundary area (B 1 ) 22 and the alloy area ( A 1 ) Easily move to 21. Here, until the time required to satisfy the low surge function elapses, the vapor pressure of the material is high and many ions and metal particles float between both contacts, and the alloy area or boundary where the arc is connected. An alloy region (A 1 ) made of a material with the lowest vapor pressure to prevent the ions and metal particles from evaporating so that the arc can be transferred while being connected between the regions, and then the high current cutoff function is satisfied.
When the arc is transferred to 21, the arc connection between both contacts is cut off at that moment.

接点が2種類の合金領域(A1)および(A2)とこれら両
領域の間の境界領域(B1)からなる場合について説明し
たが、合金領域が3種類以上存在し、それぞれの合金領
域の間に境界領域が存在する場合には、接点の半径方向
に対する蒸気圧の高さの分布の変化がより緩かなものと
なるため、アークの移行がより容易に行なわれ、停滞す
ることがない。
The case where the contact consists of two kinds of alloy areas (A 1 ) and (A 2 ) and a boundary area (B 1 ) between these areas has been described. When there is a boundary region between the contact points, the change in the distribution of the vapor pressure height in the radial direction of the contact becomes more gradual, so that the arc transition is easier and there is no stagnation. .

次に、本発明に係る接点の低サージ性および大電流しゃ
断性について試験評価した結果について説明する。それ
ぞれの接点の有する低サージ機能、大電流しゃ断機能を
比較対照するため、両接点間を接触した状態における接
点圧、この状態から離していくときの開極スピード、真
空度を同一条件とした。
Next, the results of test evaluation of the low surge property and the large current interruption property of the contact according to the present invention will be described. In order to compare and contrast the low surge function and large current interruption function of each contact, the contact pressure when both contacts were in contact, the contact opening speed when separating from this state, and the vacuum degree were the same conditions.

低サージ性の優劣は、離れている両接点間にアークが接
続されるために必要な電流さい断値の大小により評価す
ることができ、この値が小さいほど低サージ性に優れる
こととなる。LC回路を介し、44AのAC電流を与えたと
き、真空しゃ断器に直列に挿入した同軸シャントの電圧
降下をオシロスコープで測定し、電流さい断値を算出し
た。
The superiority or inferiority of the low surge property can be evaluated by the magnitude of the current interruption value required for the arc to be connected between the separated contacts, and the smaller the value, the better the low surge property. When an AC current of 44 A was applied through the LC circuit, the voltage drop of the coaxial shunt inserted in series with the vacuum breaker was measured with an oscilloscope to calculate the current interruption value.

大電流しゃ断性の優劣は、しゃ断直後におけるしゃ断性
を阻害するアークが発生しない場合における、電流の最
大値により評価することができ、この値が大きいほど大
電流しゃ断性に優れることとなる。接点表面をベーキン
グ、電圧エージング等によりクリーニングして条件を一
定にした後、7.2KV、50Hzで1KAずつ電流を増加しながら
しゃ断限界時における電流の最大値を測定し、所定の標
準値に対する倍率をしゃ断倍率として算出した。
The superiority or inferiority of the large current cutoff property can be evaluated by the maximum value of the current when an arc that inhibits the cutoff property does not occur immediately after the cutoff, and the larger this value, the better the large current cutoff property. After cleaning the contact surface by baking, voltage aging, etc. to make the conditions constant, measure the maximum value of the current at the cutoff limit while increasing the current by 1 KA at 7.2 KV, 50 Hz, and multiply the specified standard value. It was calculated as the cutoff ratio.

以上の各接点に対するサージ電流値およびしゃ断倍率を
示した表1を参照し、本発明による接点の有する効果に
ついて説明する。実施例1および従来例1はいずれも低
蒸気圧性材料の30Ag-WC-0.2Coを合金領域(A1)に、高
蒸気圧性材料の40Ag-WC-10Coを合金領域(A2)を用いて
おり、実施例1のみ境界領域(B1)を有する。この結果
しゃ断する際に最初にアークが接続されるのは、実施例
1と従来例1の両者とも同一材料からなる合金領域
(A2)であるため、電流さい断値は同一であり、低サー
ジ性に差異は見られない。ところが、実施例1は従来例
1と異なり境界領域(B1)を有するため、合金領域
(A2)から合金領域(A1)へのアークの移行が停滞する
ことなく容易に行なわれ、しゃ断倍率が1.0から1.4へ向
上している。このことは実施例2と従来例2、実施例3
と従来例3、実施例4と従来例4のいずれの関係につい
てもあてはまる。以上の試験結果から、蒸気圧の高さの
異なる材料を用いた合金領域を単に二種類以上有するだ
けでなく、各合金領域の間に蒸気圧の高さが半径方向に
対して連続して異なる分布を有する境界領域を有した本
発明による接点は、低サージ機能のみならず、大電流し
ゃ断機能をも有することが実証された。
The effect of the contact according to the present invention will be described with reference to Table 1 showing the surge current value and the breaking ratio for each contact. In both Example 1 and Conventional Example 1, 30Ag-WC-0.2Co, which is a low vapor pressure material, is used in the alloy region (A 1 ), and 40Ag-WC-10Co, which is a high vapor pressure material, is used in the alloy region (A 2 ). Therefore, only Example 1 has a boundary region (B 1 ). As a result, at the time of breaking, the arc is first connected to the alloy region (A 2 ) made of the same material in both Example 1 and Conventional Example 1, so that the current breaking value is the same, There is no difference in surge characteristics. However, unlike Example 1 of the prior art, Example 1 has a boundary region (B 1 ), so that the arc transfer from the alloy region (A 2 ) to the alloy region (A 1 ) can be easily performed without stagnation. Magnification has increased from 1.0 to 1.4. This is because the second embodiment, the second prior art, and the third embodiment.
And the relationship between Conventional Example 3 and Example 4 and Conventional Example 4 are applicable. From the above test results, not only are there two or more alloy regions that use materials with different vapor pressure heights, but the vapor pressure heights between the alloy regions are continuously different in the radial direction. It has been demonstrated that the contact according to the invention with a boundary region with distribution has not only a low surge function, but also a high current interruption function.

〔発明の効果〕 以上説明したように、本発明による真空開閉器用接点
は、低サージ機能を有する高蒸気圧性材料からなる合金
領域と、大電流しゃ断機能を有する低蒸気圧性材料から
なる合金領域とを少なくとも2種類有し、それぞれの合
金領域の間に蒸気圧の高さの半径方向の分布が連続して
異なる境界領域を有する。このため、高蒸気圧性材料か
らなる合金領域から低蒸気圧性材料からなる合金領域へ
の縦磁界の制御による強制的なアークの移行が容易に行
なわれて停滞することがなく、低サージ機能と大電流し
ゃ断機能という二つの相反する要求を同時に満たすこと
ができる。
[Effects of the Invention] As described above, the contact for a vacuum switch according to the present invention has an alloy region made of a high vapor pressure material having a low surge function and an alloy region made of a low vapor pressure material having a large current interruption function. There are at least two types, and there is a boundary region between the alloy regions in which the distribution of the vapor pressure height in the radial direction is continuously different. Therefore, forcible arc transfer is easily performed by controlling the longitudinal magnetic field from the alloy region made of the high vapor pressure material to the alloy region made of the low vapor pressure material, and it does not stagnate. It is possible to simultaneously satisfy two contradictory requirements of the current cutoff function.

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

第1図は本発明の真空開閉器用接点の一実施例を示す
図、第2図は本発明の真空開閉器用接点を製造するとき
に用いる金型の一例を示す図、第3図は成型体の中心軸
方向の断面を示す図、第4図は真空開閉器を示す図、第
5図は第4図における可動電極8周辺の詳細を示す部分
拡大図、第6図は従来の真空開閉器用接点を示す図、第
7図は真空開閉器に用いられるコイル電極を示す図、第
8図は真空開閉器に用いられるスパイラル電極を示す図
である。 1……しゃ断室、2……絶縁容器、3a,3b……封止金
具、4a,4b……金属製蓋体、5,6……導電棒、7……固定
電極、8……可動電極、9……ベローズ、10,11……ア
ークシールド、12,14……ろう付、13a……可動接点、13
b……固定接点、14……ろう付部、21……第1の合金領
域(A1)、22……第1の境界領域(B1)、23……第2の
合金領域(A2)、31……金型、32……第1のポンチ、32
a……第1のポンチの底部、32b……テーパ部、35……第
2のポンチ、35a……第2のポンチの底部、37……金型
台、38……空間、39……成型体、44……コイル電極、45
……スパイラル電極、H……磁界。
FIG. 1 is a diagram showing an embodiment of a contact for a vacuum switch of the present invention, FIG. 2 is a diagram showing an example of a die used when manufacturing the contact for a vacuum switch of the present invention, and FIG. 3 is a molded body. FIG. 4 is a view showing a cross section in the direction of the central axis of FIG. 4, FIG. 4 is a view showing a vacuum switch, FIG. 5 is a partially enlarged view showing details around the movable electrode 8 in FIG. 4, and FIG. 6 is a conventional vacuum switch. FIG. 7 is a diagram showing contacts, FIG. 7 is a diagram showing coil electrodes used in a vacuum switch, and FIG. 8 is a diagram showing spiral electrodes used in a vacuum switch. 1 ... Cutoff chamber, 2 ... Insulation container, 3a, 3b ... Sealing metal fittings, 4a, 4b ... Metal lid, 5,6 ... Conductive rod, 7 ... Fixed electrode, 8 ... Movable electrode , 9 ...... Bellows, 10, 11 ...... Arc shield, 12, 14 ...... Brazing, 13a ...... Moving contact, 13
b …… fixed contact, 14 …… brazing part, 21 …… first alloy area (A 1 ), 22 …… first boundary area (B 1 ), 23 …… second alloy area (A 2). ), 31 …… Mold, 32 …… First punch, 32
a ...... bottom of first punch, 32b ... tapered portion, 35 ... second punch, 35a ... bottom of second punch, 37 ... mold base, 38 ... space, 39 ... molding Body, 44 ... coil electrode, 45
… Spiral electrode, H… magnetic field.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】2種類の合金領域とその間にはさまれた境
界領域が同心円状に配され、前記合金領域の各々が蒸気
圧の高さの異なる材料から成り、前記境界領域が半径方
向に蒸気圧の高さが連続して異なるように組成された材
料から成ることを特徴とする真空開閉器用接点。
1. Two kinds of alloy regions and a boundary region sandwiched between the alloy regions are concentrically arranged, each of the alloy regions is made of a material having a different vapor pressure, and the boundary regions are radially arranged. A contact for a vacuum switch, characterized in that the contact is made of a material having a composition of continuously varying vapor pressures.
JP10158487A 1987-04-24 1987-04-24 Contact for vacuum switch Expired - Lifetime JPH0777101B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10158487A JPH0777101B2 (en) 1987-04-24 1987-04-24 Contact for vacuum switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10158487A JPH0777101B2 (en) 1987-04-24 1987-04-24 Contact for vacuum switch

Publications (2)

Publication Number Publication Date
JPS63266720A JPS63266720A (en) 1988-11-02
JPH0777101B2 true JPH0777101B2 (en) 1995-08-16

Family

ID=14304432

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10158487A Expired - Lifetime JPH0777101B2 (en) 1987-04-24 1987-04-24 Contact for vacuum switch

Country Status (1)

Country Link
JP (1) JPH0777101B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08249991A (en) * 1995-03-10 1996-09-27 Toshiba Corp Contact electrode for vacuum valve
JP2010251079A (en) * 2009-04-15 2010-11-04 Mitsubishi Electric Corp Switch
JP5523594B2 (en) * 2013-02-06 2014-06-18 三菱電機株式会社 Switch
JP6323578B1 (en) 2017-02-02 2018-05-16 株式会社明電舎 Electrode material manufacturing method and electrode material

Also Published As

Publication number Publication date
JPS63266720A (en) 1988-11-02

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