JPS6188414A - Vacuum circuit breaker electrode - Google Patents

Vacuum circuit breaker electrode

Info

Publication number
JPS6188414A
JPS6188414A JP20867184A JP20867184A JPS6188414A JP S6188414 A JPS6188414 A JP S6188414A JP 20867184 A JP20867184 A JP 20867184A JP 20867184 A JP20867184 A JP 20867184A JP S6188414 A JPS6188414 A JP S6188414A
Authority
JP
Japan
Prior art keywords
wire
electrode
circuit breaker
strand
vacuum circuit
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
JP20867184A
Other languages
Japanese (ja)
Inventor
古白川 信孝
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP20867184A priority Critical patent/JPS6188414A/en
Publication of JPS6188414A publication Critical patent/JPS6188414A/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】 〔産業上の利用分野〕 この発明はアークに対して概略平行な磁界を発生するよ
うに構成された真空遮断器の電極に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates to an electrode for a vacuum circuit breaker configured to generate a magnetic field substantially parallel to an arc.

〔従来の技術〕[Conventional technology]

真空遮断器の電極としては、特公昭47−30786に
示すものが提案されているか、アークに平行な磁界を印
加するように構成されていないので、遮断性能を向上さ
せることができながった。
As electrodes for vacuum circuit breakers, the one shown in Japanese Patent Publication No. 47-30786 has been proposed, and because the electrodes are not configured to apply a magnetic field parallel to the arc, the breaking performance cannot be improved. .

第7図及び第8図はアークに平行な磁界を発生するよう
にした従来の真空しゃ断器の電極を示している。図にお
いて、(1)は導電棒、(2)は導電棒(11の基部よ
り半径方向へ腕部が伸び、1ターンのコイルを経て接続
部(4)を介してアーク電極(3)へ達するコイル電極
である。(5)は非磁性で且つ高抵抗金属からなるスペ
ーサである。(Alは図示されない対向電極との間に発
生したアーク、(1)はその時流れ−る電流で、矢印に
よりその電流径路を示している。
7 and 8 show conventional vacuum breaker electrodes that generate a magnetic field parallel to the arc. In the figure, (1) is a conductive rod, (2) is a conductive rod (the arm extends radially from the base of 11, passes through one turn of the coil, reaches the arc electrode (3) via the connection part (4)) It is a coil electrode. (5) is a spacer made of non-magnetic and high resistance metal. (Al is an arc generated between the counter electrode (not shown), and (1) is a current flowing at that time, which is indicated by an arrow. The current path is shown.

次に、動作について説明する。アーク電極(3)上に発
生したアーク(Alは、その電流(1)が接続部(4)
を経て、コイル電極+21により形成された1ターンコ
イルに流れ込み導電棒(1)に達する電流経路により、
アーク(Alに平行な磁界を発生するものである。
Next, the operation will be explained. The arc (Al) generated on the arc electrode (3) causes the current (1) to flow to the connection part (4).
Through the current path that flows into the one-turn coil formed by the coil electrode +21 and reaches the conductive rod (1),
Arc (generates a magnetic field parallel to Al).

この磁界によってアーク(Alをアーク電極(3)の面
上に、無数の細い糸状のアークとして均一に分散させ、
消弧しようとするものである。
This magnetic field uniformly disperses the arc (Al) on the surface of the arc electrode (3) as countless thin thread-like arcs,
This is an attempt to extinguish the arc.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の電極は以上のように構成されていたので、コイル
電極(2:の外周部でコイルを形成しているために、半
径方向に不均一な磁界分布となることか避けられないと
いう欠点があった。又、電流通路が接続部(4)ならび
にコイル電極(2)で制限されているとともに距離が長
いため(二内部抵抗が大きく、大電流通電時には過熱す
るという欠点があった。
Conventional electrodes were constructed as described above, but because the coil is formed at the outer periphery of the coil electrode (2), it has the disadvantage that it inevitably results in uneven magnetic field distribution in the radial direction. In addition, since the current path is limited by the connection part (4) and the coil electrode (2) and the distance is long (2), there is a drawback that the internal resistance is large and overheating occurs when a large current is applied.

さらに、アーク電極(3)が薄いために機械的強度が低
く、構造複雑で高価であるなどの欠点があった。
Furthermore, since the arc electrode (3) is thin, it has low mechanical strength, has a complicated structure, and is expensive.

この発明は上記のような問題点を解消するため(=なさ
れたもので、半径方向に均一な又は任意の磁界分布が得
られて遮断性能を向上できるとともに、電流容量が太き
(て簡単な構造で機械的強度の高い、安価な真空遮断器
の電極を得ることを目的とする。
This invention was made in order to solve the above-mentioned problems, and it is possible to obtain a uniform or arbitrary magnetic field distribution in the radial direction to improve the interrupting performance, as well as to increase the current capacity (and easily The purpose is to obtain an inexpensive vacuum circuit breaker electrode with a high mechanical strength structure.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る真空遮断器の電極は、外周が電気伝導度
の低い被覆部材で覆われた線材で第1の素線を形成し、
複数本の第1の素線な束ねてねじって第2の素線を構成
し、第2の素線の先端にアーク電極を配置したものであ
る。
In the electrode of the vacuum circuit breaker according to the present invention, the first wire is formed of a wire whose outer periphery is covered with a coating member having low electrical conductivity,
A plurality of first strands are bundled and twisted to form a second strand, and an arc electrode is arranged at the tip of the second strand.

〔作用〕[Effect]

この発明における真空遮断器の電極は線材を流、 れる
電流によって、アーク(:平行な方向の磁界が発生する
The electrodes of the vacuum circuit breaker in this invention generate an arc (magnetic field in a parallel direction) by the current flowing through the wire.

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

以下、この発明の実施例を図について説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図及び第2図において、(61は良導電材からなる
主成分の線材、(7)は主成分の線材(6)を覆い、こ
の線材(6)よりも電気伝導度の低い第一の副成分から
なる被覆部材である。線材(6)と被覆部材(7)とで
第1の素線(8)を構成している。(9)は第1の素線
(8)を多数束ねた後、らせん状(二ねじられた概略コ
イル状の第2の素線である。+21は第2の素線(9)
を複数個束ねて構成されたコイル電極である。(3)は
コイル電極(21の上面を覆うように設けられたアーク
電極である。(101は導電棒(11とコイル電極(2
)との閂に設けられた、良導電材からなる接続板である
In Figures 1 and 2, (61 is a main component wire made of a highly conductive material, (7) is a first wire that covers the main component wire (6), and has a lower electrical conductivity than this wire (6). The wire rod (6) and the covering member (7) constitute the first strand (8).(9) is a covering member made of sub-components of After bundling, the second strand is shaped like a spiral (two-twisted roughly coiled wire. +21 is the second strand (9)
It is a coil electrode constructed by bundling multiple pieces. (3) is an arc electrode provided to cover the upper surface of the coil electrode (21). (101 is a conductive rod (11) and a coil electrode (21).
) is a connecting plate made of a highly conductive material and installed on the bolt.

本発明は以上のように構成されているため、導電棒[1
1から供給される電流(1)は、接続板001.コイル
電極(21を介してアーク電極(31に流されるが、コ
イル電極(2)を流れる電流の大部分は被覆部材(7)
よりも電気伝導度の良い線材(61に流れる。また、こ
の場合、第2の素線(91が概略コイル状とされている
ために、らせん状を描いているので、線材+6+ +=
流れる電流もらせん状を描き、このために軸方向すなわ
ちアークに平行な方向の磁界成分か発生し、アーク(A
)をアーク電極(3)の面上に分散させることができ、
遮断性能の向上をはかることができる。
Since the present invention is configured as described above, the conductive rod [1
The current (1) supplied from connection plate 001. The current flowing through the coil electrode (21) is passed through the arc electrode (31), but most of the current flowing through the coil electrode (2) is passed through the coating member (7).
In this case, since the second strand (91) is roughly coiled, it has a spiral shape, so the wire +6+ +=
The flowing current also draws a spiral shape, and therefore a magnetic field component is generated in the axial direction, that is, parallel to the arc, and the arc (A
) can be dispersed on the surface of the arc electrode (3),
It is possible to improve the interrupting performance.

又、はぼ電極全面が電流通路となるために過熱の恐れの
ない電流容量の大きな電極構造となっている。さらに、
第2の素線(9)のねじる度合を変化させること(−よ
って任意の磁界強度を得ることができるとともC:、ね
じる度合の異なる第2の素線(91を組み合わせて電極
を構成することにより、任意の磁界分布を得ることがで
きる。
Furthermore, since the entire surface of the electrode serves as a current path, the electrode structure has a large current capacity without fear of overheating. moreover,
By changing the degree of twist of the second wire (9) (-therefore, an arbitrary magnetic field strength can be obtained), and by combining the second wires (91) with different degrees of twist to form an electrode. By doing so, an arbitrary magnetic field distribution can be obtained.

さらにアーク電極(3)とコイル電極(21が密着して
いるために機械的強度が高くなっている。
Furthermore, since the arc electrode (3) and the coil electrode (21) are in close contact with each other, the mechanical strength is high.

また、上記実施例では第2の素線(91を複数個組み合
わせてコイル電極(2)を構成したものを示したが、第
3図、第4図(二示すごとく、第2の素線t91単体で
コイル電極を構成しても良ぐ、この場合、任意の磁界強
度分布は得られないが構造が簡単になる効果がある。さ
らに第5図に示すごとく、線状部材を線材で形成しても
良い。さらに第6図に示すごとく、第2の素線(91を
、径の異なる第1の素線(8)を組み合わせて構成して
も良く、第1の素線(810間の隙間に第1の素線(8
)よりも融点の低い充填部材αυを充填しても良い。第
8図に示したものと同様の思想で、コイル電極(2)を
径の異なる第2の素線(9)を組み合わせて構成しても
良く、また、第2の素線(91の間の隙間に第1の素線
(8)よりも融点の低い充填部材(11)を充填しても
良い。
Further, in the above embodiment, the coil electrode (2) was constructed by combining a plurality of second wires (91), but as shown in FIGS. 3 and 4 (2), the second wire t91 The coil electrode may be composed of a single coil electrode. In this case, although an arbitrary magnetic field strength distribution cannot be obtained, the structure becomes simpler.Furthermore, as shown in Fig. 5, the linear member may be formed of a wire rod. Furthermore, as shown in FIG. Insert the first strand (8
) may be filled with a filling member αυ having a lower melting point than the filling member αυ. With the same idea as shown in FIG. 8, the coil electrode (2) may be constructed by combining a second wire (9) with a different diameter, The gap may be filled with a filling member (11) having a melting point lower than that of the first wire (8).

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば、線材の外周を電気伝導
度の低い被覆部材で覆って、多数本束ねてらせん状にね
じってコイル電極を構成してアークに概略平行な磁界を
発生するようにしたので、任意の磁界強度ならびに任意
の磁界強度分布を得ることができ、遮断性能の向上をは
かることができる。又、電流容量が大きく、機械的強度
の高い、簡単な構造の電極構造を得る効果かある。
As described above, according to the present invention, the outer periphery of the wire is covered with a coating member having low electrical conductivity, and a large number of wires are bundled and twisted in a spiral to form a coil electrode, thereby generating a magnetic field approximately parallel to the arc. Therefore, any magnetic field strength and any magnetic field strength distribution can be obtained, and the interruption performance can be improved. Further, it has the effect of obtaining a simple electrode structure with a large current capacity and high mechanical strength.

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

第1図はこの発明の一実施例の正面図、第2区は第1図
の■−■断面平面図、第3図はこの発明の一実施例の正
面図、第4図は第3図のIV −IV断面平面図、第5
図は線状部材で被覆部材を構成した第1の素線の平面図
、第6図は径の異なる第1の素線で構成した第2の素線
の平面図である。第7図は従来の真空遮断器の電極の正
面図、第8図は第7図の平面図、図中(3)はアーク電
極、(6)は線材、(7)は被覆部材、(8)は第1の
素線、+91は第2の素線、住υは充填部材である。 なお、各図中同一符号は同−又は相当部分を示す。
Figure 1 is a front view of an embodiment of this invention, Section 2 is a cross-sectional plan view taken along the line ■--■ of Figure 1, Figure 3 is a front view of an embodiment of this invention, and Figure 4 is Figure 3. IV-IV cross-sectional plan view of 5th
FIG. 6 is a plan view of a first wire whose covering member is made of a linear member, and FIG. 6 is a plan view of a second wire which is made of first wires having different diameters. Fig. 7 is a front view of the electrode of a conventional vacuum circuit breaker, Fig. 8 is a plan view of Fig. 7, in which (3) is the arc electrode, (6) is the wire, (7) is the covering member, (8 ) is the first strand, +91 is the second strand, and υ is the filling member. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (7)

【特許請求の範囲】[Claims] (1)真空容器内に配置され接触面が突合されるものに
おいて、良導電性の線材の外周を上記線材より電気伝導
度の低い被覆部材で覆って第1の素線を形成し、上記第
1の素線を複数本束ねてらせん状にねじって第2の素線
を構成し、上記第2の素線の先端側を覆うように上記第
2の素線と電気的に接続されたアーク電極を設け、後端
側を電気的に短絡したことを特徴とする真空遮断器の電
極。
(1) In a device that is placed in a vacuum container and whose contact surfaces are abutted, the outer periphery of a highly conductive wire is covered with a covering member having lower electrical conductivity than the wire to form a first element wire, and the A second strand is formed by bundling a plurality of first strands and twisting them into a spiral shape, and an arc electrically connected to the second strand so as to cover the tip side of the second strand. An electrode for a vacuum circuit breaker, characterized in that an electrode is provided and the rear end side is electrically short-circuited.
(2)第2の素線は1個であることを特徴とする特許請
求の範囲第1項記載の真空遮断器の電極。
(2) The electrode for a vacuum circuit breaker according to claim 1, wherein the number of the second strands is one.
(3)第2の素線は複数個有することを特徴とする特許
請求の範囲第1項記載の真空遮断器の電極。
(3) The electrode for a vacuum circuit breaker according to claim 1, characterized in that the second wire has a plurality of pieces.
(4)第2の素線は第1の素線をねじる度合が少なくと
も2種類あることを特徴とする特許請求の範囲第3項記
載の真空遮断器の電極。
(4) The electrode for a vacuum circuit breaker according to claim 3, wherein the second wire has at least two different degrees of twisting the first wire.
(5)第2の素線は断面形状が円形でかつ径を互に異に
した複数組あることを特徴とする特許請求の範囲第3項
記載の真空遮断器の電極。
(5) The electrode for a vacuum circuit breaker according to claim 3, wherein the second wire has a circular cross-sectional shape and includes a plurality of sets having mutually different diameters.
(6)第1の素線は断面形状が円形でかつ径を互に異に
した複数組あることを特徴とする特許請求の範囲第1項
〜第6項のいずれかに記載の真空遮断器の電極。
(6) The vacuum circuit breaker according to any one of claims 1 to 6, characterized in that the first wire has a circular cross-sectional shape and there are a plurality of sets having different diameters. electrode.
(7)真空容器内に配置され接触面が突合されるものに
おいて、良導電性の線材の外周を上記線材より電気伝導
度の低い被覆部材で覆って第1の素線を形成し、上記第
1の素線を多数本束ねてらせん状にねじって第2の素線
を構成し、上記各第2の素線間に上記第1の素線よりも
低融点の充填材を充填し、上記線材の先端側に上記接触
面を形成し後端側を電気的に短絡したことを特徴とする
特許請求の範囲第1項記載の真空断断器の電極。
(7) In a device that is placed in a vacuum container and whose contact surfaces are abutted, a first strand is formed by covering the outer periphery of a highly conductive wire with a covering member having lower electrical conductivity than the wire; A second strand is formed by bundling a large number of strands of strands 1 and twisting them into a spiral shape, and a filler having a lower melting point than that of the first strand is filled between each of the second strands. 2. The electrode for a vacuum breaker according to claim 1, wherein the contact surface is formed on the leading end of the wire, and the rear end is electrically short-circuited.
JP20867184A 1984-10-04 1984-10-04 Vacuum circuit breaker electrode Pending JPS6188414A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20867184A JPS6188414A (en) 1984-10-04 1984-10-04 Vacuum circuit breaker electrode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20867184A JPS6188414A (en) 1984-10-04 1984-10-04 Vacuum circuit breaker electrode

Publications (1)

Publication Number Publication Date
JPS6188414A true JPS6188414A (en) 1986-05-06

Family

ID=16560128

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20867184A Pending JPS6188414A (en) 1984-10-04 1984-10-04 Vacuum circuit breaker electrode

Country Status (1)

Country Link
JP (1) JPS6188414A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014533427A (en) * 2011-11-15 2014-12-11 イートン コーポレーションEaton Corporation Vacuum switch and its electrode assembly

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2014533427A (en) * 2011-11-15 2014-12-11 イートン コーポレーションEaton Corporation Vacuum switch and its electrode assembly

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