JPS61110924A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS61110924A
JPS61110924A JP23126984A JP23126984A JPS61110924A JP S61110924 A JPS61110924 A JP S61110924A JP 23126984 A JP23126984 A JP 23126984A JP 23126984 A JP23126984 A JP 23126984A JP S61110924 A JPS61110924 A JP S61110924A
Authority
JP
Japan
Prior art keywords
contact
electrode
circuit breaker
coil
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
JP23126984A
Other languages
Japanese (ja)
Inventor
佐藤 能也
悟 柳父
徹 玉川
英治 金子
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 JP23126984A priority Critical patent/JPS61110924A/en
Publication of JPS61110924A publication Critical patent/JPS61110924A/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】 〔発明の技術分野〕 本発明は、真空遮断器に係p、特+1iElj構造の改
良6二関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an improvement in the structure of a vacuum circuit breaker.

〔発明の技術的背景とての問題点〕[Problems with the technical background of the invention]

周知のようにへ空越所器は、真空中で接点を開離し、A
空の優れた絶縁性能および消弧性能によυ電流をj4断
するものでめる。真空i4@器の性能は、近年、大きく
同上し、それ口ともない大隠流を通電遮断するよう(ニ
なっていり。真空遮断器の大容瀘化);ともない通磁時
の#着を防止することが必要となり、このため1:、y
til(Cu) −ビスマス(B1)材(以下Cu −
Bi材という)から形成された接触子が使用でれている
As is well known, a vacuum cleaner opens the contacts in a vacuum and
It is designed to cut off υ current by J4 due to its excellent insulation performance and arc extinguishing performance. In recent years, the performance of the vacuum i4@ has greatly improved, and it has gradually become possible to cut off large hidden currents (increasingly. Vacuum circuit breakers have a large capacity); it also prevents # adhesion during energization. Therefore, 1:,y
til (Cu) - bismuth (B1) material (hereinafter referred to as Cu -
Contactors made of Bi material (also called Bi material) have been used.

以下、この従来の真空遮断器を図面を3照して説明する
。第4図において、真空容器1は、ガラスまたはセラミ
ック等の材料から円筒状砿=形成さ・れた絶縁筒2の両
端を、金属材から形成された端板3.4で封止して構成
されたもので、この真空容器1内に、銅(Cu)材(以
下Cu材という)から形成され接離自在とした一対の電
極5,6が配設されている。しかして、11L極5は、
一端を端板3;;一体的)−接続され71c固尼通−4
4d17の他端に設は之コイル試極8に七気的に接続さ
れ、F[億6は、一端をベローズ9を介して端板4に袖
方向の移動を自在に接続された可動通電軸10の他端に
設けたコイル電極11に磁気的に接続されている。
This conventional vacuum circuit breaker will be explained below with reference to the drawings. In FIG. 4, a vacuum container 1 is constructed by sealing both ends of an insulating tube 2 formed from a material such as glass or ceramic into a cylindrical shape with end plates 3.4 formed from a metal material. In this vacuum vessel 1, a pair of electrodes 5 and 6 made of a copper (Cu) material (hereinafter referred to as Cu material) and capable of coming into contact with and separating from them are arranged. However, 11L pole 5 is
One end is connected to the end plate 3 (integral) - 71c solid - 4
The other end of 4d17 is connected to the coil test electrode 8, and the movable current-carrying shaft is connected at one end to the end plate 4 via the bellows 9 so as to be movable in the sleeve direction. It is magnetically connected to a coil electrode 11 provided at the other end of the coil electrode 10 .

これら電極5,6の中央部(:は、Cu −Bi材から
形成された接触子12.13が固着されており、この接
触子12.13は、4極面から突出した構造となってい
る。なお、同図中14はアークシールドである。ところ
で、このように構成された従来の真空遮断器C二は、欠
の欠点がある。
A contact 12.13 made of Cu-Bi material is fixed to the central part of these electrodes 5 and 6 (:), and this contact 12.13 has a structure that protrudes from the quadrupole surface. Note that 14 in the figure is an arc shield.However, the conventional vacuum circuit breaker C2 configured in this manner has a drawback of lacking.

(1)  Cu −Bi材から形成さJした接触子が、
耐斌圧峙性;二劣る。
(1) A contact made of Cu-Bi material,
Resistance to crushing pressure: 2nd inferior.

(2)投入通4時に、コイル電極を経て電流が流れるた
め犬4流の場合に、このコイル電極での通路抵抗)二よ
る温度上昇が高く、大礪流通礒が困難である。
(2) Since current flows through the coil electrode when the coil is turned on, the temperature rise due to passage resistance at this coil electrode is high and it is difficult to conduct a large current.

〔発明の目的〕[Purpose of the invention]

本発明は、上記し几事情に踵みてなさ匹たもので、電極
が溶着することなく、ま之、投入時の犬砿流通短を可能
とした真空遮断器を提供することを目的とする。
The present invention has been made in consideration of the above-mentioned circumstances, and it is an object of the present invention to provide a vacuum circuit breaker that does not cause welding of the electrodes and can shorten the flow of the wire at the time of input.

〔発明の概要〕[Summary of the invention]

本発明は、絶縁円節の両端(一端板を設けて構j戊した
真空容器内に、接離自在とした一対の電極を配設する真
空遮断器において、電極を、中心にビスマス(Bi )
の含有量が1電、t%未満の銅(Cu) −ビスマス(
Bi )材から形成された接触子を配設し、この接触子
の外側にクローム(Cr)の含有量25〜60重jt%
の鋼(Cu)−クローム(Cr)材から形成した環状部
材を端面に設けたコイル電極で構成することにより、投
入時は相互の接触子が接触して犬砥流の通磁を可能とし
、遮断時はアーク電圧の差によりアークが環状部材に移
ってコイル電極に峨流が流れ、縦磁界を発生して!l!
li性能を向上し、また、溶着(ユよる遮断不能をなく
したものである。
The present invention relates to a vacuum circuit breaker in which a pair of electrodes that can be freely connected and separated is disposed in a vacuum vessel configured by providing both ends (one end plate) of an insulating circular segment, with the electrodes being made of bismuth (Bi) at the center.
Copper (Cu)-bismuth (with a content of less than 1 t%)
A contact made of Bi) material is disposed, and a chromium (Cr) content of 25 to 60% by weight is placed on the outside of this contact.
By constructing an annular member made of steel (Cu) and chromium (Cr) material with coil electrodes provided on the end face, the mutual contactors come into contact with each other at the time of injection, enabling magnetic conduction in a dogtooth style. At the time of interruption, the arc moves to the annular member due to the difference in arc voltage, and a torrent flows to the coil electrode, generating a vertical magnetic field! l!
This improves LI performance and eliminates the inability to shut off due to welding.

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

以下、本発明の真空遮断器の一実施例を図面を参照して
説明する。なお、従来の真空遮断器においては、固定電
極と可動電極で構成の相違するものもあるが、この実施
例では両電極に同じ構成であるから、以下の説明は可m
Nm+二ついて行なう。
Hereinafter, one embodiment of the vacuum circuit breaker of the present invention will be described with reference to the drawings. In addition, in some conventional vacuum circuit breakers, the fixed electrode and the movable electrode have different configurations, but in this example, both electrodes have the same configuration, so the following explanation can be used.
Perform with Nm + two.

第11Aおよび第2図;=おいて、可動電極加は、1重
量%未溝のBiを含むCu−B1材から形成され、0電
動通礁@9の上端の凹tiβ9a i二凸部21aを挿
入してロー付は等で固着さ才L7’Cs触子4部21、
この接触子基部21と同一のCu −Bi材から形成さ
れ、接触子基部21の上部の凹部21bに凸snaを挿
入してロー付は等で固着した接触子n、この接触子nと
同心円状(ユ装置され、上端面を接触子乙の上端面より
1〜2朋低くし、かつ5〜60重−t%のクローA (
Cr)を含む銅(Cu)−クローム(Cr)材(以下C
u −Cr材という)から形成された接点部材お、この
接点部材乙を上部の凹部24aに挿入してロー付は等で
固着した4極夙、この電極24の裏面側1−間隔をもっ
て配置され、可動通電軸91:峨気的に接続さ才すたコ
イル電極5、例えばステンレス鋼のような低導峨材から
形成され、下部をコイル電極5に固着し上部がi硫億ム
に当償するスペーサが、このスベー?あと同一の低導也
材から形成され、下部を可動通電軸9に支持され上部が
コイル4.極δに固着されたコイル4惚支持部材nから
構成されている。
11A and FIG. Insert and solder the L7'Cs contactor 4 part 21,
A contact n made of the same Cu-Bi material as this contact base 21, with a convex SNA inserted into the recess 21b at the top of the contact base 21 and fixed with brazing, etc., is formed in a concentric circle with this contact n. (The upper end surface is 1 to 2 mm lower than the upper end surface of the contact element B, and the claw A of 5 to 60 weight-t% (
Copper (Cu)-chromium (Cr) material (hereinafter referred to as C
A contact member made of a Cr material is inserted into the upper recess 24a, and the four electrodes are fixed with brazing or the like, and the contact member B is arranged at a distance of 1 on the back side of the electrode 24. , movable current-carrying shaft 91: electrically connected to the coil electrode 5, made of a low conductivity material such as stainless steel, with the lower part fixed to the coil electrode 5 and the upper part connected to the coil electrode 5. Is this a good spacer? It is also made of the same low conductivity material, with the lower part supported by the movable current-carrying shaft 9 and the upper part supported by the coil 4. It consists of a coil support member n fixed to the pole δ.

ここで、コイル電極西は、可動通1軸9の上部のコイル
取付部25aにロー付は等で固着されかつ半径方向に伸
びる腕部25b lニ一端が固着され、他端が七の上面
でかつ腕部25bの近傍の礪匝ムの裏面側と接続部25
cを介して固着し、断面が四角形(ただし外側の下方角
部のみ円弧状ンの清拭材を外注が(憾囚と略等しくなる
ような円弧状に形成した円弧部25dから構成さ才し、
−面側をコイル礒憚支持部材!に支持されている。また
、コイル電極支持部材27は、例えばステンレス鋼のよ
うな低導屯材から形成され、可動通(軸9に獣会し固着
する基部77a、この2′7aと同一の低導(材から形
成され、基部27a(ニ一端を固着され等間隔に配置さ
れて半径方向に伸びる複数の支持腕部27bから構成さ
れ、この支持腕部2′7bの他端がコイル電極5の円弧
部25d;二固着される。
Here, the coil electrode west is fixed to the coil mounting part 25a on the upper part of the movable shaft 9 by brazing or the like, and has one end fixed to the arm part 25b extending in the radial direction, and the other end is fixed to the upper surface of the shaft 9. and the back side of the tumbler near the arm portion 25b and the connecting portion 25
The wiping material is fixed through the cylindrical part 25c and has a rectangular cross section (however, only the outer lower corner has an arc-shaped cleaning material). ,
- The coil support member is on the side! is supported by The coil electrode support member 27 is made of a low-conductivity material such as stainless steel, and has a base 77a that is fixed to the shaft 9 and is made of the same low-conductivity material as the base 77a, which is fixed to the shaft 9. It is composed of a plurality of support arms 27b fixed at one end of the base 27a and extending in the radial direction and arranged at equal intervals. Fixed.

さらに、接点部材るおよび電極24には、接触子基部■
および接触子乙の外径よフ2〜3龍大きい内径の穴21
aおよび22bがそれぞれ設けられ、接触子基部21お
よび接触子nと隙間G (1〜1,5罷)が形成されて
いる。法た、複数の半径方向に伸びるスリット29が設
けられている。
Furthermore, the contact member and the electrode 24 have a contact base ■
and a hole 21 with an inner diameter 2 to 3 times larger than the outer diameter of the contact piece.
a and 22b are provided, respectively, and a gap G (1 to 1,5 lines) is formed with the contact base 21 and the contact n. At the bottom, a plurality of radially extending slits 29 are provided.

次に、上記構成の作用を説明する。操作機構(:より可
動通硫軸9が移動して可m胤極美が固足磁億(図示しな
い)に道触した状態、すなわち投入状態においては、外
ftf5回路からの電流は、固定電極(図示しない)か
ら接触子22. ffl触子基部21、可動通硫軸9を
径て外m回路へ通電する。ここで、コイル竜他25には
、接触子nおよび接触子基部21が直接接触せず、しか
も接触子nが接点部材乙および電極かより突出していて
相手側とも接触しないので、磁流は通電しない。つtシ
、固建礒惚(図示しない)と可動電極Iは、それぞれの
接触子nのみを介して通電し、それぞれのコイル電極6
には通電しない。したがって、投入状態(−おいて、コ
イル電極50通路抵抗によシ温度上昇することはなく、
大砥流の通電に何ら支障はない。
Next, the operation of the above configuration will be explained. When the operating mechanism (:) moves the movable sulfur shaft 9 and the movable shaft 9 touches the fixed foot magnet (not shown), that is, in the closed state, the current from the outer FTF5 circuit is transferred to the fixed electrode. (not shown) to the outer m circuit via the contactor 22.ffl contactor base 21 and the movable sulfur shaft 9.Here, the contactor n and the contactor base 21 are connected directly to the coil dragon 25. They do not contact each other, and since the contact n protrudes from the contact member A and the electrode and does not contact the other side, no magnetic current is applied. energized only through each contact n, each coil electrode 6
does not turn on. Therefore, in the closed state (-), the temperature does not rise due to the passage resistance of the coil electrode 50,
There is no problem in energizing the large whirlpool.

次に、操作機構により可動通磁軸9が上記と反対方向に
移動して可動@極美が固厘覗極(図示しない)から離間
する場合、固定電極(図示しない)と可動環+jA20
の当初の接触部分μCu −Bi材から形成され九それ
ぞれの接触子aであったから、Cu −Bi材の#看引
外し力が比較的小さく、小さい引外し力で固imm<図
示しない)と可動電極美を離間できる。したがって、溶
着現Rによる遮断不能は発生しない。なお、遮断により
それぞれの接触子nの接触面に接点部材温を形成するC
u材、やCr材の薄膜が形成されても、接触子nの母材
がCu −Bi材であるため溶着による遮断不能は防止
できる。また、可動電憔加が固足尾極(図示しない)か
ら離間すると、Cu −Bi材から形成された接触子η
上(ニアークが発生する。ここで、接触子n上に発生し
たアークのカソードスポットは、1箇所のみ口とどま′
ることなくその一部はCu −Cr材から形成された接
点部材23にも移動し、アノード側には複離した磁子や
イオンが接触子nや接点部材23(ニ一様に拡が9流れ
込む。そこで、接点部材乙、電極屑、コイル4極25に
も通磁し、同時(−コイル(極δの腕部δbを流れるル
ープ磁流により、電極屑平面に直交する磁界(以下縦磁
界という)を発生する。ここで、コイル電極5の外径が
電極屑の外径より小さ過ぎると、4他面中央の縦磁界の
みが強くなり、コイル電極5の外側では磁界は弱くなっ
て方向が逆転してしまい、可動電極美と固足颯極(図示
しない)間に発生したアークが接点部材nおよび電極屑
の表面上(ニ一様に広がらずに果申してしまう。また、
コイル電極δの外径が電極屑の外径よυ大き過ぎると、
コイル!也25 により発生する縦磁界の強度が弱く、
第3図に示すアーク磁圧と縦磁界の関係における最小ア
ーク電圧値に連する程の縦磁界が得られず、すなわち、
アーク電圧を降下させることはできない。
Next, when the operating mechanism moves the movable magnetizing shaft 9 in the opposite direction to the above and the movable @Gokumi is separated from the fixed electrode (not shown) and the fixed electrode (not shown) and the movable ring +jA20
Since the initial contact portion of μCu-Bi material was formed of each contact a, the pulling force of the Cu-Bi material was relatively small, and the small tripping force made it rigid and movable. Electrode beauty can be separated. Therefore, failure to shut off due to welding R does not occur. In addition, C which forms a contact member temperature on the contact surface of each contactor n by interruption
Even if a thin film of U material or Cr material is formed, since the base material of contact n is Cu--Bi material, failure to shut off due to welding can be prevented. Moreover, when the movable electric force is separated from the fixed foot tail pole (not shown), the contact η formed from Cu-Bi material
Upper (near arc occurs. Here, the cathode spot of the arc generated on the contact n remains at only one location.
Some of them also move to the contact member 23 made of Cu-Cr material, and on the anode side, the decoupled magnetons and ions are transferred to the contact n and the contact member 23 (uniformly spread 9 Therefore, the contact member B, the electrode scrap, and the 4-pole coil 25 are also energized, and at the same time (- coil (-), due to the loop magnetic current flowing through the arm part δb of the pole δ, a magnetic field perpendicular to the plane of the electrode scrap (hereinafter referred to as longitudinal magnetic field) is generated. Here, if the outer diameter of the coil electrode 5 is too small than the outer diameter of the electrode scrap, only the vertical magnetic field at the center of the 4th surface will be strong, and the magnetic field will be weaker on the outside of the coil electrode 5 and will not change in the direction. is reversed, and the arc generated between the movable electrode and the solid foot pole (not shown) spreads over the surface of the contact member n and the electrode scrap (without spreading evenly. Also,
If the outer diameter of the coil electrode δ is too large than the outer diameter of the electrode scrap,
coil! 25 The strength of the longitudinal magnetic field generated by
A longitudinal magnetic field comparable to the minimum arc voltage value in the relationship between arc magnetic pressure and longitudinal magnetic field shown in FIG. 3 cannot be obtained, that is,
It is not possible to reduce the arc voltage.

したがって、コイル電極5の外径は、電極屑の外径の0
.5@以上でかつ1.5倍以下でなければならない。さ
ら口、可動電極美と固足醋極(図示しない)間(ニ一様
な縦磁界を発生させるためには、単一のコイル電極では
不充分であυ可属υ電極美および固疋鳳他(図示しない
)にそれぞれ同一のコイル電極を設け、かつ各コイル(
極の円弧g25di=流れる4流による等制約なワンタ
ーンの閉ループ(流は、同一円周方向となるようにしな
けlしばならない。第3図に示すように、縦磁界の磁束
冨度が増大、つまシ縦磁界の強さが増大するとアークシ
圧は、最小アーク電圧1直まで減少し、その後徐々に増
大するV特性を示す。なお、弗3図に示す曲線刃はCu
材、曲線31はCu−Cr材のV特性を示す。
Therefore, the outer diameter of the coil electrode 5 is equal to 0 of the outer diameter of the electrode scrap.
.. Must be 5@ or more and 1.5 times or less. In order to generate a uniform longitudinal magnetic field between the movable electrode and the fixed pole (not shown), a single coil electrode is insufficient. The same coil electrodes are provided in other coils (not shown), and each coil (
Polar arc g25di = One-turn closed loop with equal constraints due to four flowing flows (the flows must be in the same circumferential direction. As shown in Figure 3, the magnetic flux density of the longitudinal magnetic field increases, As the strength of the longitudinal magnetic field increases, the arc pressure decreases to the minimum arc voltage of 1 arc, and then shows a V characteristic that gradually increases.The curved blade shown in Figure 3 is Cu
Curve 31 shows the V characteristics of the Cu-Cr material.

Bi材の含有!1重量%未満のCu −Bi材は、Bi
材の含有量がatであるためにBi材のアーク1圧への
形番が小さく曲線Iと略等しくなる。したがって、カソ
ードスポットが接点部材23(−移動し、アノード側に
おける一様な拡が9の荷框粒子の流れ込みによる縦磁界
の発生によυ、Cu =−Cr材から形成された接点部
材n上に発生したアークへ圧が低くなり、かつ縦磁界の
拡散効果(;より遮断性能に曖れ再点弧発生のないCu
 −Cr材から形成された接点部材n上へアークがさら
に拡が夛、犬柩流遮断が可能となる。通常、可動側心鳳
Iが固定側電極(図示しない)と接触および離間、すな
わら投入および遮断時には、強大な償単力で投入および
引外しが行なわれる。したがって、この強大なis力が
電極24およびコイル電極25に作用するので、屯億ス
の変形を防止するだめの支持部材として、ステンレス鋼
のような低4毫材から形成されたスペーサ訪が、七の下
部をコイル取付N 25&にロー付は等により固着さオ
℃、上部を電極UのA面に当接するように設けらtてい
る。また、コイル電極6の変形を防止するための支持部
材として、 ステンレス鋼のような低導電材から形成されたコイル電
極支持部材γが、その下部を可動通磁軸9にロー付は等
により固着し、円周方向で等間隔に配置され半径方向に
伸びる複数の支持腕部27b の先端部を円弧部25d
の裏面側にロー付は等に上9固着するように設けられて
いる。ここで、スペーサがおよびコイル電極支持部材2
7は、ステンレス鋼のような低導電材から形成されてい
るので、スペーサあおよびコイル電極支持部材27に分
流される磁流はきわめて小さい。
Contains Bi material! Less than 1% by weight of Cu-Bi material is Bi
Since the content of the material is at, the model number of the Bi material to one arc pressure is small and approximately equal to curve I. Therefore, the cathode spot moves to the contact member 23 (-), and the uniform spread on the anode side is caused by the generation of a longitudinal magnetic field due to the flow of the cargo frame particles 9, onto the contact member n made of Cu=-Cr material. The pressure on the arc that occurs is lowered, and the diffusion effect of the vertical magnetic field (Cu
- The arc further spreads onto the contact member n made of Cr material, making it possible to interrupt the flow. Normally, when the movable side core I contacts and separates from the fixed side electrode (not shown), that is, when it is turned on and off, the closing and tripping are performed with a strong compensating force. Therefore, since this strong IS force acts on the electrode 24 and the coil electrode 25, a spacer made of a low-strength material such as stainless steel is used as a supporting member to prevent the force from deforming. The lower part of the coil is attached to the coil N25 by brazing, etc., and the upper part is provided so as to come into contact with the A side of the electrode U. Further, as a support member for preventing deformation of the coil electrode 6, a coil electrode support member γ made of a low conductivity material such as stainless steel is fixed at its lower part to the movable magnetic shaft 9 by brazing, etc. The tips of the plurality of support arms 27b arranged at equal intervals in the circumferential direction and extending in the radial direction are connected to the arcuate portion 25d.
A brazing plate is provided on the back side of the plate so that the upper plate 9 is fixed to the plate. Here, the spacer and the coil electrode support member 2
Since 7 is made of a low conductivity material such as stainless steel, the magnetic current that is shunted to the spacer hole and the coil electrode support member 27 is extremely small.

さらに、投入時に接触子nが強い投入力で相手側の接触
子と接触するので、軸方向(:収縮し半径方向に膨張す
るが、接点部材乙および電像あとの間に隙間Gが設けら
れており、支嘩を与えないようになっている。一方、接
点部材ると篭極冴に手径方向に伸びる複数のスリン)2
9が設けられているので、縦磁界が発生したとき縦磁界
と逆方向磁界を発生するような接点部材nおよび電極2
4に流れる!iA流等のルーグ題流を阻止し、逆磁界4
二よる縦磁界の減少を防止する。
Furthermore, when the contact n contacts the other contact with a strong closing force, it contracts in the axial direction (: contracts and expands in the radial direction), but a gap G is created between the contact member B and the electric image. On the other hand, the contact member has a plurality of sulins extending in the radial direction of the handle (2).
9 is provided, so that when a longitudinal magnetic field is generated, the contact member n and the electrode 2 generate a magnetic field in the opposite direction to the longitudinal magnetic field.
Flows to 4! Blocks Loog flow such as iA flow, reverse magnetic field 4
This prevents the vertical magnetic field from decreasing due to

なお、以上の説明においては、コイル電極5の円弧部2
5dが一体のものでめったが、円弧部25dを互に接触
しない複数に分割するとともに腕部25bも複数設け、
分割した各円弧部25dの両端をそれぞれ腕部25bに
固着し、隣接する円弧部25dの対向する端部をそれぞ
れ接続部25cを介して砿極ヌ1:固看し、各円弧部2
5d(−流れる磁流が等動的;二ワンターンの閉ループ
を形成するようにした分書l形のコイル1極としてもよ
い。
In addition, in the above description, the circular arc portion 2 of the coil electrode 5
5d is rarely integrated, but the arc part 25d is divided into a plurality of parts that do not touch each other, and a plurality of arm parts 25b are also provided.
Both ends of each divided circular arc part 25d are fixed to the arm part 25b, and the opposite ends of the adjacent circular arc parts 25d are connected to each other via the connecting part 25c.
5d (-The flowing magnetic current is equidynamic; it may be a single-pole coil with an L-shape that forms a two-turn closed loop.

〔発明の効果〕〔Effect of the invention〕

本発明は、以上のように構成されているから、迩斯性能
が優才し、1帽二よる遮断不能をなくし、投入時におけ
るコイル電極の通路抵抗による温度上昇がなく大1ム流
通覗を可能とする。
Since the present invention is constructed as described above, it has excellent flow performance, eliminates the inability to shut off due to one cap and two, and eliminates the temperature rise due to the passage resistance of the coil electrode when it is turned on, allowing for a large 1-m flow. possible.

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

第1図は本発明のJc空空所断器一実馬例の要部を示す
平面図、第2図は第1図のA−0−A線に沿って矢印1
同に見た断面図、第3図は本発明(:関連する銅と銅−
クロームの縦磁界の強さとアーク磁圧の関係を示す曲線
図、第4図は従来の真空J断器の構成を示す断面図でる
る。 1・・・真空容器、    2・・・絶縁円筒加・・・
可動電極、    21・・・接触子お・・・接点部材
、    b・・・コイル電極27・・・コイル電極支
持部材 第  1  図 第  2  図 第3図 o        o、I        O,10,
,3?ば4しイ’ifkベトごりλ1ぷ=束庇K   
ffノ第  4  図
FIG. 1 is a plan view showing the main part of a Jc hollow cutter of the present invention, and FIG. 2 is an arrow 1 along line A-0-A in FIG.
The cross-sectional view shown in FIG. 3 shows the present invention (: related copper and copper-
FIG. 4 is a curve diagram showing the relationship between the strength of the longitudinal magnetic field of chrome and the arc magnetic pressure, and FIG. 4 is a sectional view showing the structure of a conventional vacuum J-breaker. 1...Vacuum container, 2...Insulating cylinder processing...
Movable electrode, 21...Contact member...Contact member, b...Coil electrode 27...Coil electrode support member Fig. 1 Fig. 2 Fig. 3 o o, I O, 10,
,3? ba4shii'ifkstickylambda1pu=bundle K
Figure 4 of ff

Claims (5)

【特許請求の範囲】[Claims] (1)絶縁円筒の両端に端板を設けて構成した真空容器
内に、接離自在とした一対の電極を配設する真空遮断器
において、前記電極を、中心にビスマス(Bi)の含有
量が1重量%未満の銅(Cu)−ビスマス(Bi)材か
ら形成された接触子を配設し、この接触子の外側にクロ
ーム(Cr)の含有量25〜60重量%の銅(Cu)−
クロム(Cr)材から形成した環状部材を端面に設けた
コイル電極で構成したことを特徴とする真空遮断器。
(1) In a vacuum circuit breaker in which a pair of electrodes that can be freely brought into and out of contact with each other is disposed in a vacuum container configured by providing end plates at both ends of an insulating cylinder, the content of bismuth (Bi) is A contact made of a copper (Cu)-bismuth (Bi) material with a chromium (Cr) content of less than 1% by weight is provided, and copper (Cu) with a chromium (Cr) content of 25 to 60% by weight is disposed on the outside of this contact. −
A vacuum circuit breaker comprising a coil electrode having an annular member made of chromium (Cr) material on the end face.
(2)接触子を、円板状部材より突出して設けた特許請
求の範囲第1項記載の真空遮断器。
(2) The vacuum circuit breaker according to claim 1, wherein the contactor is provided to protrude from the disc-shaped member.
(3)コイル電極を、銅(Cu)より低導電材から形成
した支持部材で通電軸に支持した特許請求の範囲第1項
記載の真空遮断器。
(3) The vacuum circuit breaker according to claim 1, wherein the coil electrode is supported on the current-carrying shaft by a support member made of a material having a lower conductivity than copper (Cu).
(4)円板状部材を含むコイル電極の端面に、半径方向
に伸びる直線状のスリツトを設けた特許請求の範囲第1
項記載の真空遮断器。
(4) A linear slit extending in the radial direction is provided on the end face of the coil electrode including the disc-shaped member.
Vacuum circuit breaker as described in section.
(5)一対の電極を略同一構成とした特許請求の範囲第
1項記載の真空遮断器。
(5) The vacuum circuit breaker according to claim 1, wherein the pair of electrodes has substantially the same configuration.
JP23126984A 1984-11-05 1984-11-05 Vacuum breaker Pending JPS61110924A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23126984A JPS61110924A (en) 1984-11-05 1984-11-05 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23126984A JPS61110924A (en) 1984-11-05 1984-11-05 Vacuum breaker

Publications (1)

Publication Number Publication Date
JPS61110924A true JPS61110924A (en) 1986-05-29

Family

ID=16920957

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23126984A Pending JPS61110924A (en) 1984-11-05 1984-11-05 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS61110924A (en)

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