JPH08111148A - Vacuum valve electrode - Google Patents
Vacuum valve electrodeInfo
- Publication number
- JPH08111148A JPH08111148A JP24282494A JP24282494A JPH08111148A JP H08111148 A JPH08111148 A JP H08111148A JP 24282494 A JP24282494 A JP 24282494A JP 24282494 A JP24282494 A JP 24282494A JP H08111148 A JPH08111148 A JP H08111148A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- magnetic field
- tip
- vacuum valve
- joined
- 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.)
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Landscapes
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
Abstract
(57)【要約】
【目的】遮断性能と通電容量を上げることができる真空
バルブの電極を得ること。
【構成】通電軸17の先端に背面の中心部が接合される電
極1には、中央部から放射状に外側に形成された4本の
腕部1aを設け、この腕部1aの先端には、弧状のコイ
ル部1bを形成する。電極1の前面には、電極板3を設
け、この電極板3は、円板部3aの外周に90°間隔に突
起部3bを設け、この突起部3bをコイル部1bの先端
1cにろう付する。電極板3の前面には、接点2をろう
付する。
(57) [Summary] [Purpose] To obtain electrodes for vacuum valves that can increase the breaking performance and current carrying capacity. [Structure] The electrode 1 in which the center portion of the back surface is joined to the tip of an energization shaft 17 is provided with four arm portions 1a formed radially outward from the center portion, and the tip of this arm portion 1a is The arc-shaped coil portion 1b is formed. An electrode plate 3 is provided on the front surface of the electrode 1, and the electrode plate 3 is provided with protrusions 3b at 90 ° intervals on the outer periphery of the disc portion 3a, and the protrusions 3b are brazed to the tip 1c of the coil portion 1b. To do. The contact 2 is brazed to the front surface of the electrode plate 3.
Description
【0001】[0001]
【産業上の利用分野】本発明は、真空バルブの電極に係
り、特に、縦磁界電極の構成を変えた真空バルブの電極
に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a vacuum valve electrode, and more particularly to a vacuum valve electrode in which the structure of a longitudinal magnetic field electrode is changed.
【0002】[0002]
【従来の技術】従来の真空遮断器に組み込まれる真空バ
ルブの構成の一例を図5の縦断面図に示す。図5に示す
ように、真空バルブ10は、絶縁円筒11の両端を固定フラ
ンジ12と可動フランジ13で封止して構成される真空容器
の内部に、固定電極14と可動電極15を所定の間隙で対置
している。2. Description of the Related Art An example of the structure of a vacuum valve incorporated in a conventional vacuum circuit breaker is shown in a vertical sectional view of FIG. As shown in FIG. 5, the vacuum valve 10 includes a fixed electrode 14 and a movable electrode 15 in a predetermined space inside a vacuum container configured by sealing both ends of an insulating cylinder 11 with a fixed flange 12 and a movable flange 13. It is confronted with.
【0003】このうち、固定電極14は、固定フランジ12
の中心に貫設された銅棒製の固定通電軸16の先端に固定
され、この固定通電軸16の基端を介して真空容器の外部
と接続される。また、可動電極15は、同じく銅棒製の可
動通電軸17の先端に固定され、真空容器の外部とはこの
可動通電軸17の下部を介して接続される。Of these, the fixed electrode 14 is the fixed flange 12
It is fixed to the tip of a fixed current-carrying shaft 16 made of a copper rod penetrating the center of the vacuum vessel, and is connected to the outside of the vacuum container via the base end of the fixed current-carrying shaft 16. The movable electrode 15 is fixed to the tip of a movable energizing shaft 17 which is also made of a copper rod, and is connected to the outside of the vacuum container via the lower part of the movable energizing shaft 17.
【0004】この可動通電軸17は、可動フランジ13の中
心に挿入された軸受22を貫通し、下端が可動フランジ13
の内面にろう付されたベローズ18を介して可動フランジ
13を気密に貫通している。したがって、真空バルブは、
真空容器内の真空を維持した状態で可動通電軸17の下端
に図示しない絶縁ロッドを介して連結された図示しない
操作機構部により、可動電極15の固定電極14への接離を
可能にしている。べローズ18の上端は、上端が可動通電
軸17に接合されたべローズカバー19の上部下面にろう付
され、絶縁円筒11の内面の中央部には、円筒状のアーク
シールド20が取り付けられている。The movable energizing shaft 17 penetrates a bearing 22 inserted in the center of the movable flange 13, and the lower end thereof is movable flange 13.
Movable flange through the bellows 18 brazed to the inner surface of the
It penetrates 13 airtightly. Therefore, the vacuum valve
The movable electrode 15 can be brought into and out of contact with the fixed electrode 14 by an operation mechanism portion (not shown) connected to the lower end of the movable energizing shaft 17 via an insulating rod (not shown) while maintaining the vacuum in the vacuum container. . The upper end of the bellows 18 is brazed to the upper and lower surfaces of a bellows cover 19 whose upper end is joined to the movable energizing shaft 17, and a cylindrical arc shield 20 is attached to the center of the inner surface of the insulating cylinder 11. .
【0005】ところで、真空バルブは、真空の優れた消
弧性能と絶縁特性を利用しているため、他の絶縁媒体を
使用した、例えば、六フッ化硫黄ガスを絶縁媒体とした
遮断器に比べて、電極間の間隙を近接させることがで
き、外形を小形にすることができる。また、遮断容量に
おいても、電極の構造を以下説明するように改良するこ
とによって更に増やすことができる。By the way, since the vacuum valve utilizes the excellent arc extinguishing performance and insulating property of vacuum, compared with a circuit breaker using another insulating medium, for example, sulfur hexafluoride gas as the insulating medium. Thus, the gaps between the electrodes can be close to each other, and the outer shape can be made small. Also, the breaking capacity can be further increased by improving the structure of the electrode as described below.
【0006】真空バルブの遮断性能を上げるためには、
電極間に発生するアークによる電極の局部的な加熱を抑
える必要がある。したがって、従来から、電極の局部的
な加熱による異常な荷電粒子と金属蒸気の発生を抑える
ことができる電極の構成が研究され、且つ、実用化され
ている。このための電極構造としては、電流遮断時に電
極間に発生するアークに対して、アーク電流で発生した
磁界によって駆動力を加える方法が一般的である。In order to improve the shutoff performance of the vacuum valve,
It is necessary to suppress the local heating of the electrodes due to the arc generated between the electrodes. Therefore, conventionally, a structure of an electrode capable of suppressing abnormal generation of charged particles and metal vapor due to local heating of the electrode has been studied and put into practical use. As an electrode structure for this purpose, it is general to apply a driving force to the arc generated between the electrodes when the current is cut off by a magnetic field generated by the arc current.
【0007】この磁界の印加方法の一つとして、電極間
に発生するアークに対して、直交する方向に磁界を印加
する方法がある。この方法を採用した電極構造には、一
般的にスパイラル電極及びコントレート電極と呼ばれて
いる電極がある。このような電極で発生する磁界は、電
極の中心から放射方向の磁界である。As one of the methods of applying the magnetic field, there is a method of applying a magnetic field in a direction orthogonal to the arc generated between the electrodes. Electrode structures that employ this method include electrodes generally called spiral electrodes and contract electrodes. The magnetic field generated by such an electrode is a magnetic field in the radial direction from the center of the electrode.
【0008】したがって、電極間に発生したアークに対
して円周方向にローレンツ力が働く。この力によって、
アークは円周方向に回転駆動され、電極表面を回転す
る。アークを回転させることにより、局部的な熱入力を
防ぎ、電極の溶融を防ぐことができる。Therefore, a Lorentz force acts in the circumferential direction on the arc generated between the electrodes. By this power,
The arc is rotationally driven in the circumferential direction and rotates on the surface of the electrode. By rotating the arc, local heat input can be prevented and melting of the electrodes can be prevented.
【0009】しかし、この真空バルブを高電圧の回路を
遮断する真空遮断器に適用するためには、電極間の耐電
圧を向上させるために、電極間の距離を増やす必要があ
る。この場合に、上述した電極間に発生するアークに対
して直交する方向の磁界を印加する電極構造を用いた場
合には、アークが電極表面を回転するときに、アークが
円周方向に伸ばされ、電極の外周から放射方向に飛び出
すおそれがあるだけでなく、この飛び出たアークが、電
極の外側に取り付けられているアークシールドへ点弧す
るおそれがある。However, in order to apply this vacuum valve to a vacuum circuit breaker for breaking a high-voltage circuit, it is necessary to increase the distance between the electrodes in order to improve the withstand voltage between the electrodes. In this case, when the electrode structure for applying a magnetic field in a direction orthogonal to the arc generated between the electrodes described above is used, when the arc rotates on the electrode surface, the arc is stretched in the circumferential direction. Not only is there a possibility that the outer periphery of the electrode will be ejected in the radial direction, but this ejected arc may be ignited to the arc shield attached to the outside of the electrode.
【0010】すると、アークの脚がその双方の点弧位置
に停滞し、この部分に対して局部的に過大な熱入力が発
生する。この過大な熱入力によって電極とアークシール
ドの点弧部分が溶融し、遮断性能を低下させる。さら
に、このような電極構造では、前述したように、アーク
は高温の集中アークであるため、接触子の消耗が増え、
大電流の開閉寿命が低下する。Then, the legs of the arc are stagnated at both ignition positions, and excessive heat input is locally generated to this portion. This excessive heat input melts the electrode and the ignition part of the arc shield, and reduces the breaking performance. Furthermore, in such an electrode structure, as described above, since the arc is a high-temperature concentrated arc, the contact wear is increased,
The switching life of large current is reduced.
【0011】電流遮断時に発生するアークに対して、こ
のアークを駆動する磁界を印加する他の方法として、電
極間に発生するアークに対して、平行な軸方向の磁界、
すなわち、縦磁界を印加する方法がある。この方法を採
用した電極は、いわゆる縦磁界電極と呼ばれ、この電極
間に発生したアークは、電極の対向面の全体に均一に広
がり、電極表面の局部的な過大な熱入力を防ぎ、遮断性
能の優れた電極構造とすることができる。As another method of applying a magnetic field for driving the arc generated when the current is cut off, a magnetic field in an axial direction parallel to the arc generated between the electrodes,
That is, there is a method of applying a vertical magnetic field. The electrodes that employ this method are called so-called longitudinal magnetic field electrodes, and the arc generated between these electrodes spreads evenly over the entire opposing surface of the electrodes, preventing local excessive heat input on the electrode surface and interrupting it. An electrode structure with excellent performance can be obtained.
【0012】また、高電圧の回路に接続される真空バル
ブにおいて電極間距離を増やした場合でも、前述した縦
磁界の強度を適正に選択することにより、電極間に安定
したアークを点弧することができ、遮断性能を上げるこ
とができる。さらに、アークの点弧位置が分散するた
め、大電流遮断時においても、接触子の消耗が少なく、
開閉寿命を延ばすことができる。Even when the distance between the electrodes is increased in a vacuum valve connected to a high voltage circuit, a stable arc can be ignited between the electrodes by properly selecting the strength of the longitudinal magnetic field described above. It is possible to improve the blocking performance. Furthermore, since the ignition positions of the arc are dispersed, even when a large current is cut off, the contact wear is small,
The switching life can be extended.
【0013】代表的な軸方向の磁界を発生させる従来の
電極構造を図6の平面図で説明する。なお、図6は、接
触子を省略した状態で前面から見た図を示している。こ
の電極は、背後にコイル電極21を設け、このコイル電極
21に流れる電流により、電極間に軸方向の磁界、すなわ
ち、縦磁界を発生させる。コイル電極21に流れる電流
は、中心から90°間隔で放射状に伸びる4本の腕部21a
に分流し、各腕部21aの先端から弧状に湾曲したコイル
部21bに流れ、このコイル部21bの先端21cからこの先
端にろう付された接触子に流れる。A conventional electrode structure for generating a typical axial magnetic field will be described with reference to the plan view of FIG. It should be noted that FIG. 6 shows a view as seen from the front with the contacts omitted. This electrode is provided with a coil electrode 21 on the back, and this coil electrode 21
A current flowing in 21 generates a magnetic field in the axial direction between the electrodes, that is, a vertical magnetic field. The current flowing through the coil electrode 21 is four arm portions 21a extending radially from the center at 90 ° intervals.
Flow into the arc-shaped curved coil portion 21b from the tip of each arm 21a, and from the tip 21c of the coil 21b to the contact brazed to the tip.
【0014】このコイル電極21を可動電極側と固定電極
側の接点の後面にそれぞれ取り付け、コイル部21bに流
れる電流により電極間に前述した軸方向の磁界を発生さ
せる。なお、図6では腕部21aが4分割の場合を示して
いるが、腕部の数を変えることで、軸方向の磁界の強さ
を変えることができる。The coil electrodes 21 are attached to the rear surfaces of the contacts on the movable electrode side and the fixed electrode side, respectively, and the above-mentioned axial magnetic field is generated between the electrodes by the current flowing through the coil portion 21b. Although FIG. 6 shows the case where the arm portion 21a is divided into four, the strength of the magnetic field in the axial direction can be changed by changing the number of arm portions.
【0015】軸方向の磁界を発生させる他の電極構造と
して、特公平 3−22007 号公報に示されるように、カッ
プ状の電極の円筒部分に螺旋状のスリットを形成し、軸
方向の磁界を発生させる構造が提案されている。この電
極では、円筒部分の電流経路を螺旋状に形成することに
より、電流の円周方向の成分が発生し、これにより電極
間に軸方向の磁界を発生させる。この軸方向の磁界の強
度は、円筒部に形成されたスリットの傾きを変える等の
方法で変えることができる。As another electrode structure for generating an axial magnetic field, as shown in Japanese Patent Publication No. 32007/1990, a spiral slit is formed in the cylindrical portion of a cup-shaped electrode to generate an axial magnetic field. Structures to generate are proposed. In this electrode, by forming the current path of the cylindrical portion in a spiral shape, a circumferential component of the current is generated, thereby generating an axial magnetic field between the electrodes. The strength of the magnetic field in the axial direction can be changed by changing the inclination of the slit formed in the cylindrical portion.
【0016】[0016]
【発明が解決しようとする課題】真空遮断器を大容量の
電力系統に適用するためには、遮断容量と通電容量を増
やすことが必要となる。この要求に対して、電極の構造
と接触子材料の改良が進められ、このうち、接触子材料
としては、例えば、銅クロム合金等の特殊な合金が開発
されている。In order to apply the vacuum circuit breaker to a large capacity power system, it is necessary to increase the breaking capacity and the current carrying capacity. In response to this demand, the structure of the electrodes and the contact material have been improved, and as the contact material, a special alloy such as a copper-chromium alloy has been developed.
【0017】一方、接触子間に発生するアークと平行に
磁界を発生させる縦磁界の電極構造の研究から、磁界の
強度とアーク電圧の関係を調査した結果、ある磁界強度
でアーク電圧が最低値を示すことが明らかになってい
る。このアーク電圧が最低値を示す磁界強度を印加する
ことにより、接触子間で消費されるアークエネルギーが
最小となり、遮断性能が最高となる。On the other hand, as a result of investigating the relationship between the strength of the magnetic field and the arc voltage from the research of the electrode structure of the longitudinal magnetic field that generates a magnetic field parallel to the arc generated between the contacts, the arc voltage has the lowest value at a certain magnetic field strength. It has been revealed that By applying the magnetic field strength at which the arc voltage exhibits the lowest value, the arc energy consumed between the contacts is minimized and the breaking performance is maximized.
【0018】また、アーク電圧が最低になる磁界強度
は、電極の直径や遮断電流及び接触子材料等によって異
なり、遮断性能を上げるためには、磁界の強度を上げる
必要がある。図6に示すコイル電極を使用して、軸方向
の磁界を発生させる電極構造では、腕部21aの数を減ら
すことによって、前述した電流の弧状成分の増加で磁界
の強度を上げることができる。例えば、腕部21aの数を
4本から、3本、2本と減らすことにより、磁界の強度
は、約 1.3倍、2倍と増え、遮断条件に最適な磁界強度
とすることができ、遮断性能を上げることができる。The magnetic field strength at which the arc voltage becomes the minimum depends on the diameter of the electrode, the breaking current, the contact material, etc., and it is necessary to increase the strength of the magnetic field in order to improve the breaking performance. In the electrode structure for generating a magnetic field in the axial direction by using the coil electrode shown in FIG. 6, it is possible to increase the strength of the magnetic field by increasing the arc-shaped component of the current described above by reducing the number of the arms 21a. For example, by reducing the number of arms 21a from four to three and two, the magnetic field strength increases to about 1.3 times and two times, and it is possible to obtain the optimum magnetic field strength for the blocking condition. Performance can be improved.
【0019】しかし、このような磁界強度の増加方法で
は、通電経路が長くなるので、コイル電極部分での抵抗
が増える。これにより、通常の負荷電流を通電している
場合の温度上昇が過大となるおそれがあった。したがっ
て、腕部の数を減らした場合には、各腕部とコイル部の
断面積を増やす必要があるので、電極が大きくなるとと
もに、製作が難しく、信頼性が低下するおそれがある。However, in such a method of increasing the magnetic field strength, the current-carrying path becomes long, so that the resistance at the coil electrode portion increases. As a result, there is a possibility that the temperature rise becomes excessive when the normal load current is applied. Therefore, when the number of arms is reduced, it is necessary to increase the cross-sectional area of each arm and the coil, so that the electrode becomes large and the manufacturing is difficult, and the reliability may be reduced.
【0020】また、通電容量を増やすためにコイル部の
断面積を増やすと、同一の電極外径の場合、磁界を発生
させる部分の中心径が減少する。したがって、電極端部
における磁界が減少し、電極面全体を有効に利用するこ
とができず、遮断性能が低下するおそれがある。さら
に、電流を遮断する場合に電極間に発生するアークが電
極の端部から点弧したときに、磁界の弱い部分でアーク
が点弧するためアークが不安定となり、電極からアーク
シールド側へアークが伸び、アークの磁界による制御が
効かず、遮断性能を低下させるおそれがあった。Further, when the cross-sectional area of the coil portion is increased to increase the current carrying capacity, the center diameter of the portion that generates the magnetic field is reduced when the outer diameter of the electrode is the same. Therefore, the magnetic field at the electrode end portion decreases, the entire electrode surface cannot be effectively used, and the blocking performance may deteriorate. Furthermore, when the current is cut off, when the arc generated between the electrodes is ignited from the end of the electrode, the arc becomes unstable in the weak magnetic field and the arc becomes unstable. Was extended, the control by the magnetic field of the arc was not effective, and there was a fear that the breaking performance was deteriorated.
【0021】そこで、本発明の目的は、上記課題に鑑
み、外形を増やすことなく、遮断性能を上げ、かつ、通
電容量を増やすことのできる真空バルブの電極を得るこ
とである。Therefore, in view of the above problems, an object of the present invention is to obtain an electrode of a vacuum valve capable of improving the breaking performance and increasing the current carrying capacity without increasing the outer shape.
【0022】[0022]
【課題を解決するための手段】請求項1,2及び請求項
3に記載の発明の真空バルブの電極は、通電軸の先端に
背面の中心部が接合され、この中心部から複数の通電腕
部が放射状に形成され、この通電腕部の先端からコイル
部が弧状に形成された電極の前面に対して、複数の突起
部が円板部の外周に形成された電極板を接合し、この電
極板の前面に円板状の接点を接合したことを特徴とす
る。また、電極板の突起部はコイル部の先端に接合する
ことが好ましく、さらに、接点の断面形状は頂面の外周
が曲面となる円錐台状とし、頂部の直径をD1とし電極
板の円板部の直径をD2としたとき、D2>D1とする
ことが好ましい。In the electrodes of the vacuum valve according to the present invention as set forth in claims 1, 2 and 3, the center of the back surface is joined to the tip of the current-carrying shaft, and a plurality of current-carrying arms are provided from this center. Parts are formed in a radial shape, and a plurality of protrusions are joined to the front surface of the electrode in which the coil portion is formed in an arc shape from the tip of the energizing arm portion, and the electrode plate formed on the outer circumference of the disk portion is joined to the front surface of the electrode portion. It is characterized in that a disc-shaped contact is joined to the front surface of the electrode plate. Further, it is preferable that the protruding portion of the electrode plate is joined to the tip of the coil portion, and the cross-sectional shape of the contact is frusto-conical with the outer circumference of the top face being a curved surface, and the diameter of the top is D1 and the disc plate of the electrode plate. When the diameter of the portion is D2, it is preferable that D2> D1.
【0023】また、請求項4に記載の発明の真空バルブ
の電極は、通電軸の先端に背面の中心部が接合され、こ
の中心部の外側から複数の溝部がこの溝部の底部と通電
軸の軸心を結ぶ線に対して直交方向に放射状に形成され
た有底筒状の電極の前面に対して、複数の突起部が円板
部の外周に形成された電極板を接合し、この電極板の前
面に円板状の接点を接合したことを特徴とする。Further, in the electrode of the vacuum valve according to the fourth aspect of the present invention, the center of the back surface is joined to the tip of the current-carrying shaft, and a plurality of grooves are provided from the outside of the center to the bottom of the groove and the current-carrying shaft. An electrode plate with a plurality of protrusions formed on the outer circumference of the disk part is joined to the front surface of a bottomed cylindrical electrode that is formed radially in a direction orthogonal to the line connecting the axes, and this electrode It is characterized in that a disc-shaped contact is joined to the front surface of the plate.
【0024】[0024]
【作用】このように構成された真空バルブの電極におい
ては、電極のコイル部の軸方向の厚みを減らすことがで
き、真空バルブの内部で対置される一対の電極のコイル
部間の距離が短縮されるとともに、コイル部の電路も短
縮される。In the electrode of the vacuum valve thus constructed, the axial thickness of the coil portion of the electrode can be reduced, and the distance between the coil portions of the pair of electrodes opposed to each other inside the vacuum valve can be shortened. At the same time, the electric path of the coil portion is shortened.
【0025】[0025]
【実施例】以下、本発明の真空バルブの電極の一実施例
を図面を参照して説明する。図1は、請求項1及び請求
項2と請求項3に記載の発明の真空バルブの電極を示す
平面図で、図2は、図1のA−A断面図である。なお、
図1,図2は、可動通電軸に接合された可動電極の場合
を示し、固定電極も、可動通電軸を固定通電軸に変える
ことによって、同一構造となる。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the electrode of the vacuum valve of the present invention will be described below with reference to the drawings. FIG. 1 is a plan view showing electrodes of a vacuum valve according to the first and second and third aspects of the invention, and FIG. 2 is a sectional view taken along line AA of FIG. In addition,
1 and 2 show the case of a movable electrode joined to a movable current-carrying shaft, and the fixed electrode also has the same structure by changing the movable current-carrying shaft to the fixed current-carrying shaft.
【0026】図1及び図2において、可動通電軸17の先
端にろう付れた縦磁界電極1の上面には、円板状の外周
に突起部3bが90°間隔に突設された電極板3がろう付
され、この電極板3の上面には、円板状の接点2がろう
付されている。In FIGS. 1 and 2, on the upper surface of the vertical magnetic field electrode 1 brazed to the tip of the movable energizing shaft 17, projections 3b are provided on the disk-shaped outer periphery at intervals of 90 °. 3 is brazed, and a disc-shaped contact 2 is brazed to the upper surface of the electrode plate 3.
【0027】このうち、縦磁界電極1は、図2に示す縦
断面の形状が浅いU字状に形成され、図1の平面図にお
いては、従来の技術で示した図6の電極と同様に、90°
間隔に中央部から放射状に形成された腕部1aと、この
腕部1aの先端に連続して形成された弧状のコイル部1
bで構成されている。Of these, the longitudinal magnetic field electrode 1 is formed in a shallow U-shape in the longitudinal section shown in FIG. 2, and in the plan view of FIG. 1, it is the same as the electrode of FIG. 6 shown in the prior art. , 90 °
Arm portions 1a radially formed from the central portion at intervals and an arc-shaped coil portion 1 continuously formed at the tip of the arm portion 1a.
b.
【0028】したがって、図6で示した電極21と異なる
ところは、図6で示したコイル部21bの先端の上面側に
形成された先端21cが省かれているだけで、他は同一で
ある。すなわち、コイル部1bの上面は、基部から先端
まで平面である。Therefore, the difference from the electrode 21 shown in FIG. 6 is the same except that the tip 21c formed on the upper surface side of the tip of the coil portion 21b shown in FIG. 6 is omitted. That is, the upper surface of the coil portion 1b is a flat surface from the base portion to the tip.
【0029】また、電極板3は、この電極板3の直径D
1で示す円板部3aの外周に突設された前述した突起部
3bが、コイル1bの先端の前面に重ねられてろう付さ
れている。なお、 180°に対置した突起部3bの外周面
間の寸法(すなわち、突起部3bの先端を結ぶ円の直
径)は、縦磁界電極1の外径と同一である。The electrode plate 3 has a diameter D of the electrode plate 3.
The above-mentioned protrusion 3b protruding from the outer periphery of the disc portion 3a indicated by 1 is brazed on the front surface of the tip of the coil 1b. The dimension between the outer peripheral surfaces of the protrusions 3b opposite to each other at 180 ° (that is, the diameter of the circle connecting the tips of the protrusions 3b) is the same as the outer diameter of the vertical magnetic field electrode 1.
【0030】また、接点2は、図2で示した縦断面の形
状が偏平な台形で、外径は、縦磁界電極1及びこの縦磁
界電極1の上面にろう付された電極板3の突起部3b間
の距離と同一である。台形状の接点2の上辺となる可動
通電軸17とほぼ同径の直径D2の平面部分と、この外周
の斜面部との間に形成された鈍角部は、アークの膠着を
防ぐために面取りされて曲面となっている。The contact 2 has a trapezoidal shape having a flat vertical cross section as shown in FIG. 2, and the outer diameter is a protrusion of the vertical magnetic field electrode 1 and the electrode plate 3 brazed to the upper surface of the vertical magnetic field electrode 1. It is the same as the distance between the parts 3b. An obtuse angle portion formed between a flat surface portion having a diameter D2 having substantially the same diameter as that of the movable energization shaft 17 which is an upper side of the trapezoidal contact 2 and a slope portion of the outer periphery is chamfered to prevent arc sticking. It is a curved surface.
【0031】次に、このように構成された真空バルブの
電極の作用を説明する。可動通電軸17から接点2に流れ
る電流は、可動通電軸17の先端に接続された縦磁界電極
1から電極板3を経て接点2に流れ、この接点2の表面
から、この接点2と対向して設けられた固定側電極の接
点に流れる。Next, the operation of the electrodes of the vacuum valve thus constructed will be described. The current flowing from the movable energizing shaft 17 to the contact 2 flows from the longitudinal magnetic field electrode 1 connected to the tip of the movable energizing shaft 17 to the contact 2 through the electrode plate 3, and the surface of the contact 2 opposes the contact 2. Flows to the contact of the fixed side electrode that is provided.
【0032】このうち、縦磁界電極1に流れる電流は、
腕部1aからコイル部1bに流れる。このコイル部1b
を流れる電流は、このコイル部1bの先端前面にろう付
された電極板3の突起部3bから接点2に流れる。する
と、コイル部1bに流れる電流は、図1の平面図におい
ては弧状で且つアークと直交方向となるので、このコイ
ル部1bに流れる電流によって発生した磁束は、遮断時
において一対の接点間に発生したアークに対して平行な
縦磁界となる。Of these, the current flowing through the vertical magnetic field electrode 1 is
It flows from the arm portion 1a to the coil portion 1b. This coil part 1b
The electric current flowing through the coil portion 1b flows from the protrusion 3b of the electrode plate 3 brazed to the front surface of the tip of the coil portion 1b to the contact 2. Then, the current flowing through the coil portion 1b has an arc shape in the plan view of FIG. 1 and is in a direction orthogonal to the arc. Therefore, the magnetic flux generated by the current flowing through the coil portion 1b is generated between the pair of contacts at the time of interruption. A longitudinal magnetic field parallel to the arc is generated.
【0033】このように構成された真空遮断器の電極に
おいては、縦磁界の強度は、縦磁界電極1に形成された
コイル部1bの数を変えることによって、遮断電流に対
応した最適値に変えることができることは前述したとお
りである。In the electrode of the vacuum circuit breaker thus constructed, the strength of the longitudinal magnetic field is changed to an optimum value corresponding to the breaking current by changing the number of coil portions 1b formed in the longitudinal magnetic field electrode 1. What can be done is as described above.
【0034】また、従来の真空バルブの電極において
は、通電容量を増やすために腕部1aとコイル部1bの
軸方向の厚さを増やした場合には、固定電極に組み込ま
れたコイル部1bと可動電極に組み込まれたコイル部1
bの相互間の距離が増えるので、それだけアークに対す
る縦磁界の強度が低下していた。しかるに、本発明の真
空バルブの電極においては、図6で示した先端21cによ
る軸方向の突起がなく、それだけコイル部1bの相互間
の距離が接近するので、逆にアークに対する縦磁界を増
やすことができる。In the conventional vacuum valve electrode, when the axial thickness of the arm portion 1a and the coil portion 1b is increased in order to increase the current carrying capacity, the coil portion 1b incorporated in the fixed electrode is Coil part 1 incorporated in the movable electrode
Since the distance between b is increased, the strength of the longitudinal magnetic field with respect to the arc is reduced accordingly. However, in the electrode of the vacuum valve of the present invention, there is no projection in the axial direction due to the tip 21c shown in FIG. 6, and the distance between the coil portions 1b becomes closer to that much, so conversely increase the longitudinal magnetic field for the arc. You can
【0035】したがって、対向した一対の電極間の距離
が短縮されることによって、真空バルブの長さを減らす
ことができるだけでなく、遮断性能を上げることができ
る。さらに、先端21cを省略することによって、電極の
形状が簡単となり製作が容易となるだけでなく、コイル
部の電路が短縮されるので、コイル部の抵抗値の減少に
よって、このコイル部に起因する温度上昇を防ぐことが
でき、通電容量を増やすことができる。Therefore, by shortening the distance between the pair of electrodes facing each other, not only the length of the vacuum valve can be reduced but also the breaking performance can be improved. Further, by omitting the tip 21c, not only the shape of the electrode is simplified and the manufacturing is facilitated, but also the electric path of the coil portion is shortened, so that the resistance value of the coil portion is reduced, which causes the coil portion. It is possible to prevent temperature rise and increase current carrying capacity.
【0036】さらに、接点2は、直径D1の広い接合面
積の円板部3aを備えた電極板3にろう付されるので、
接合強度を上げることができ、投入時の衝撃に耐え、且
つ、僅かな撓みによる接触面のなじみによって相互の接
触面積が広くなり、接触抵抗を減らし、この接触抵抗の
減少により温度上昇も減らすことができ、したがって通
電容量も増やすことができる。Further, since the contact 2 is brazed to the electrode plate 3 having the disk portion 3a having a large joint area with the diameter D1,
The joint strength can be increased, it can withstand impact at the time of injection, and the contact surface becomes small due to the bending of the contact surfaces to widen the mutual contact area, reducing the contact resistance, and reducing this contact resistance also reduces the temperature rise. Therefore, the current-carrying capacity can be increased.
【0037】次に、請求項4に記載の発明の真空バルブ
の電極の一実施例を図3とこの図3の前面図を示す図4
で説明する。図3及び図4において、図1及び図2と異
なるところは、縦磁界電極1Aと、この縦磁界電極1A
の上面の電極板3の更に上面にろう付された接点2Aの
形状である。Next, an embodiment of the electrode of the vacuum valve of the invention according to claim 4 is shown in FIG. 3 and a front view of FIG.
Described in. 3 and FIG. 4 are different from FIG. 1 and FIG. 2 in that a vertical magnetic field electrode 1A and a vertical magnetic field electrode 1A are provided.
The shape of the contact 2A brazed to the upper surface of the upper electrode plate 3 of FIG.
【0038】すなわち、縦磁界電極1Aには、図1にお
いては底部の中心の外側の部分から放射状に且つ対称的
に4条の溝1dが形成されている。これらの溝1dは、
縦磁界電極1Aの外周に抜け、更に図2の正面図におい
て右上方に傾斜して上端に開口部を形成している。ま
た、この開口部の左側に鋭角の先端部1c1をそれぞれ
形成している。That is, in the longitudinal magnetic field electrode 1A, in FIG. 1, four grooves 1d are formed radially and symmetrically from a portion outside the center of the bottom. These grooves 1d are
It goes out to the outer periphery of the vertical magnetic field electrode 1A, and further, in the front view of FIG. Further, an acute-angled tip portion 1c1 is formed on the left side of this opening.
【0039】縦磁界電極1Aの上面にろう付される電極
板3は、この電極板3の外周に突設された突起部3bが
縦磁界電極1Aの外周に形成された先端部1c1の上面
と重なるように設けられている。一方、接点2Aは、接
触面の大部分が平面で、外周部に僅かに曲面部が形成さ
れている。The electrode plate 3 to be brazed on the upper surface of the vertical magnetic field electrode 1A has a projection 3b projecting on the outer periphery of the electrode plate 3 and an upper surface of a tip 1c1 formed on the outer periphery of the vertical magnetic field electrode 1A. It is provided so as to overlap. On the other hand, in the contact point 2A, most of the contact surface is a flat surface, and a slightly curved surface portion is formed on the outer peripheral portion.
【0040】このように可動電極と固定電極が構成され
た真空バルブにおいても、通電電流は、可動通電軸17か
ら縦磁界電極1Aを経て電極板3の突起部3bから接点
2Aに流れ、この過程において、縦磁界電極1Aに形成
された溝1dにより、この縦磁界電極1Aの中心部から
外周の先端部1c1に弧状に流れる電流によって、縦磁
界が発生する。Even in the vacuum valve having the movable electrode and the fixed electrode as described above, the energizing current flows from the movable energizing shaft 17 through the longitudinal magnetic field electrode 1A to the contact portion 2A from the protrusion 3b of the electrode plate 3 and this process. In, the longitudinal magnetic field is generated by the groove 1d formed in the longitudinal magnetic field electrode 1A by the arc-shaped current flowing from the central portion of the longitudinal magnetic field electrode 1A to the tip portion 1c1 of the outer periphery.
【0041】この場合には、図1及び図2で示した電極
と比べて、可動通電軸17から各先端部1c1に流れる弧
状の電路の断面積と、接点相互の接触面積を増やすこと
ができるので、通電容量を更に増やし、電極の温度上昇
を更に減らすことができる利点がある。In this case, compared with the electrodes shown in FIGS. 1 and 2, it is possible to increase the cross-sectional area of the arc-shaped electric path flowing from the movable energization shaft 17 to each tip 1c1 and the contact area between the contacts. Therefore, there is an advantage that the current carrying capacity can be further increased and the temperature rise of the electrode can be further reduced.
【0042】[0042]
【発明の効果】以上、請求項1,2及び請求項3に記載
の発明によれば、通電軸の先端に背面の中心部が接合さ
れ、この中心部から複数の通電腕部が放射状に形成さ
れ、この通電腕部の先端からコイル部が弧状に形成され
た電極の前面に対して、複数の突起部が円板部の外周に
形成された電極板を接合し、この電極板の前面に円板状
の接点を接合することで、電極の軸方向の厚みを減ら
し、真空バルブの内部で対置される一対の電極のコイル
部間の距離を減らしたので、外形を増やすことなく、遮
断性能と通電容量を上げることのできる真空バルブの電
極を得ることができる。As described above, according to the inventions of claims 1, 2 and 3, the central portion of the back surface is joined to the tip of the current-carrying shaft, and a plurality of current-carrying arm portions are radially formed from this central portion. Then, from the tip of this energizing arm portion, to the front surface of the electrode in which the coil portion is formed in an arc shape, the electrode plate having the plurality of protrusions formed on the outer circumference of the disc portion is joined, and the front surface of this electrode plate is joined. By connecting the disc-shaped contacts, the axial thickness of the electrodes was reduced, and the distance between the coil parts of the pair of electrodes opposite each other inside the vacuum valve was reduced. Thus, it is possible to obtain an electrode of a vacuum valve capable of increasing the current carrying capacity.
【0043】また、請求項4に記載の発明によれば、通
電軸の先端に背面の中心部が接合され、この中心部の外
側から複数の溝部がこの溝部の底部と前記通電軸の軸心
を結ぶ線に対して直交方向に放射状に形成された有底筒
状の電極の前面に対して、複数の突起部が円板部の外周
に形成された電極板を接合し、この電極板の前面に円板
状の接点を接合することで、電極の軸方向の厚みを減ら
し、真空バルブの内部で対置される一対の縦磁界を発生
させる電路間の距離を減らしたので、外形を増やすこと
なく、遮断性能と通電容量を上げることのできる真空バ
ルブの電極を得ることができる。Further, according to the invention described in claim 4, the center portion of the back surface is joined to the tip of the current-carrying shaft, and a plurality of groove portions are provided from the outside of the center portion so as to form the bottom portion of the groove portion and the axis of the current-carrying shaft. To the front surface of the bottomed tubular electrode that is radially formed in a direction orthogonal to the line connecting the electrode plates, the electrode plate having a plurality of protrusions formed on the outer periphery of the disk part is joined, and By connecting a disc-shaped contact to the front surface, the axial thickness of the electrode was reduced, and the distance between the electric paths that generated a pair of longitudinal magnetic fields opposite each other inside the vacuum valve was reduced. Without, it is possible to obtain an electrode of a vacuum valve capable of increasing the breaking performance and the current carrying capacity.
【0044】[0044]
【図1】請求項1,2及び請求項3に記載の発明の真空
バルブの電極の一実施例を示す平面図。FIG. 1 is a plan view showing an embodiment of electrodes of a vacuum valve of the invention according to claims 1, 2 and 3.
【0045】[0045]
【図2】図1のA−A断面図。FIG. 2 is a sectional view taken along line AA of FIG.
【0046】[0046]
【図3】請求項3に記載の発明の真空バルブの電極の一
実施例を示す平面図。FIG. 3 is a plan view showing an embodiment of an electrode of the vacuum valve according to the invention of claim 3;
【0047】[0047]
【図4】図3の前面図。FIG. 4 is a front view of FIG.
【0048】[0048]
【図5】従来の真空バルブの電極が組み込まれた真空バ
ルブの一例を示す縦断面図。FIG. 5 is a vertical sectional view showing an example of a vacuum valve in which electrodes of a conventional vacuum valve are incorporated.
【0049】[0049]
【図6】従来の真空バルブの電極の要部を示す平面図。FIG. 6 is a plan view showing a main part of an electrode of a conventional vacuum valve.
【0050】[0050]
1,1A…縦磁界電極、1a…腕部、1b…コイル部、
1c,1c1…先端部、1d…溝,2,2A…接点、3
…電極板、3a…円板部、3b…突起部、17…可動通電
軸。1, 1A ... Longitudinal magnetic field electrode, 1a ... Arm portion, 1b ... Coil portion,
1c, 1c1 ... Tip, 1d ... Groove, 2, 2A ... Contact point, 3
... electrode plate, 3a ... disk part, 3b ... projection part, 17 ... movable energizing shaft.
Claims (4)
この中心部から複数の通電腕部が放射状に形成され、こ
の通電腕部の先端からコイル部が弧状に形成された電極
と、この電極の前面に接合され複数の突起部が円板部の
外周に形成された電極板と、この電極板の前面に接合さ
れる円板状の接点でなる真空バルブの電極。1. The center of the back surface is joined to the tip of the current-carrying shaft,
A plurality of energizing arms are radially formed from this center part, and an electrode in which a coil part is formed in an arc shape from the tip of this energizing arm part, and a plurality of protrusions joined to the front surface of this electrode are the outer circumference of the disc part. An electrode of a vacuum valve, which is composed of an electrode plate formed on the substrate and a disc-shaped contact point joined to the front surface of the electrode plate.
たことを特徴とする請求項1に記載の真空バルブの電
極。2. The electrode of a vacuum valve according to claim 1, wherein the projection of the electrode plate is joined to the tip of the coil.
円錐台状とし、頂部の直径をD1とし、電極板の円板部
の直径をD2としたとき、D2>D1としたことを特徴
とする請求項1又は請求項2に記載の真空バルブの電
極。3. The cross-sectional shape of the contact is frustoconical in which the outer circumference of the top surface is a curved surface, the diameter of the top portion is D1, and the diameter of the disc portion of the electrode plate is D2, D2> D1. The electrode of the vacuum valve according to claim 1 or 2, characterized in that.
この中心部の外側から複数の溝部がこの溝部の底部と前
記通電軸の軸心を結ぶ線に対して直交方向に放射状に形
成された有底筒状の電極と、この電極の前面に接合され
複数の突起部が円板部の外周に形成された電極板と、こ
の電極板の前面に接合される円板状の接点でなる真空バ
ルブの電極。4. The center of the back surface is joined to the tip of the current-carrying shaft,
A plurality of groove portions are joined from the outside of the center portion to a bottomed cylindrical electrode radially formed in a direction orthogonal to a line connecting the bottom portion of the groove portion and the axis of the current-carrying shaft and the front surface of the electrode. An electrode of a vacuum valve, which is composed of an electrode plate having a plurality of protrusions formed on the outer periphery of the disc part and a disc-shaped contact point joined to the front surface of the electrode plate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24282494A JPH08111148A (en) | 1994-10-06 | 1994-10-06 | Vacuum valve electrode |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24282494A JPH08111148A (en) | 1994-10-06 | 1994-10-06 | Vacuum valve electrode |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH08111148A true JPH08111148A (en) | 1996-04-30 |
Family
ID=17094843
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24282494A Pending JPH08111148A (en) | 1994-10-06 | 1994-10-06 | Vacuum valve electrode |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH08111148A (en) |
-
1994
- 1994-10-06 JP JP24282494A patent/JPH08111148A/en active Pending
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