JPS59230226A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS59230226A
JPS59230226A JP10449983A JP10449983A JPS59230226A JP S59230226 A JPS59230226 A JP S59230226A JP 10449983 A JP10449983 A JP 10449983A JP 10449983 A JP10449983 A JP 10449983A JP S59230226 A JPS59230226 A JP S59230226A
Authority
JP
Japan
Prior art keywords
coil
vacuum
magnetic field
electrodes
center
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
JP10449983A
Other languages
Japanese (ja)
Inventor
芦沢 喬
佐野 孝光
川上 秀雄
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.)
Meidensha Corp
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Corp
Meidensha Electric Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Meidensha Corp, Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Corp
Priority to JP10449983A priority Critical patent/JPS59230226A/en
Publication of JPS59230226A publication Critical patent/JPS59230226A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は真空しゃ断器番ζ係り、特にしゃ断時において
発生したアークに、このアークと同方向の磁界を印加す
るよう化した真空しゃ断器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum breaker number ζ, and more particularly to a vacuum breaker that applies a magnetic field in the same direction as the arc generated during the breaker.

従来、しゃ断時において一対の電極間化生じたアーク−
こ、このアークと同方向の磁界(所謂縦磁界)を印加さ
せてしゃ断能力の向上を図った真空提 しゃ断器が数多く損案されているが、この種真空しゃ断
器は、開閉部となる真空インタラプタlこ一体的に磁界
発生用のコイルを装着せしめて成るのが一般的であり、
このような真空インタラプタを大別すると、第1図に示
すような真空容器内にコイルを備えたものと、第2図に
示すような真空容器外にコイルを備えたものとに別ける
ことができる。
Conventionally, the arc that occurs between a pair of electrodes during interruption
There have been many proposals for vacuum circuit breakers in which the breaking ability is improved by applying a magnetic field in the same direction as the arc (so-called longitudinal magnetic field). Interrupters are generally equipped with a coil for generating a magnetic field,
Broadly speaking, such vacuum interrupters can be divided into those that have a coil inside the vacuum container as shown in Figure 1, and those that have a coil outside the vacuum container as shown in Figure 2. .

すなわち、第1図の真空インタラプタは、絶鎌筒の両端
を金属端板番こより閉塞してなる真空容器1内に1対の
導電棒2 ’ # 2 bを相対的に接近離反自在に導
入するとともに、各導電棒2a、2bの内端部に電極3
 a、、 3 bを絶縁スペーク4a。
That is, in the vacuum interrupter shown in FIG. 1, a pair of conductive rods 2'#2b are introduced into a vacuum container 1 formed by closing both ends of a cylindrical cylinder with metal end plates so that they can approach and separate from each other. At the same time, an electrode 3 is provided at the inner end of each conductive rod 2a, 2b.
a, , 3 b insulating space 4a.

4bを介して機械的に固着し、各導電棒2a、2bとそ
れぞれの電極3a、3bとを各電極3a、3bの背部に
配設されかつ導電棒2a、2bに流れる軸方向の電流を
導電棒2a、2bを中心とするループ電流に変更して縦
磁界を発生するコイル5a。
4b, each conductive rod 2a, 2b and each electrode 3a, 3b are arranged on the back of each electrode 3a, 3b, and conducts an axial current flowing through the conductive rod 2a, 2b. A coil 5a generates a longitudinal magnetic field by changing the current to a loop centered around the rods 2a and 2b.

5bを介し電気的に接続して構成されている。They are configured to be electrically connected via 5b.

そして、上記真空インタラプタは、絶縁フレーム(図示
省略)に収納されるとともに、各導電棒2 a # 2
bの外端部に、主回路導体(図示省略)と接離される端
子導体6a、6bが接続され、かつベローズ7を介し移
動自在な導電棒2bを駆すべく操作装置(図示省略)が
付設されて真空しゃ断器として構成されている。
The vacuum interrupter is housed in an insulating frame (not shown), and each conductive rod 2a #2
Terminal conductors 6a and 6b that connect and separate from the main circuit conductor (not shown) are connected to the outer end of b, and an operating device (not shown) is attached to drive the movable conductive rod 2b via the bellows 7. It is configured as a vacuum breaker.

ところが、第1図の真空インタラプタにあっては、次の
ような欠点がある。
However, the vacuum interrupter shown in FIG. 1 has the following drawbacks.

■ コイル5a、5bが真空容器1内に設けられている
ため、流通電流によりコイル5 a * 5 bに生ず
るジュール熱を外部に放散しにくい。
(2) Since the coils 5a and 5b are provided within the vacuum vessel 1, it is difficult to dissipate the Joule heat generated in the coils 5a*5b due to the flowing current to the outside.

■ 導電棒の内端部に、電極3a、3bの他に絶縁スペ
ーサ4a、4bおよびコイ#5a、5’b等の複数の部
材をろう付により固着しているため、可動部の重量増大
をもたらし、特に大容量用のものにあっては、操作時の
操作力および衝撃が大となるとともに耐久性の低下をも
たらしている。
■ In addition to the electrodes 3a and 3b, multiple members such as insulating spacers 4a and 4b and coil #5a and 5'b are fixed to the inner end of the conductive rod by brazing, which reduces the weight of the movable parts. In particular, in the case of large-capacity devices, the operating force and impact during operation are large, and durability is reduced.

■ コイル5a、5bが電極3 a * 3 bの背部
に設けられているため、電極3a、3bの開離にしたが
ってアークに印加される縦磁界の強度低下をもたらし、
拡散しているアークが磁界強度の低下に伴って集中化し
てしゃ断能力に悪影響を及ぼすという問題がある。
■ Since the coils 5a and 5b are provided on the back of the electrodes 3a*3b, the strength of the longitudinal magnetic field applied to the arc decreases as the electrodes 3a and 3b separate,
There is a problem in that the diffused arc becomes concentrated as the magnetic field strength decreases, which adversely affects the breaking ability.

以上の如く第1図に示す真空インタラプタにあっては、
しゃ断能力におのずと限界があり、比較的低容量のもの
には適するものの、高容量のものには向かないことが分
ってきた。
As mentioned above, in the vacuum interrupter shown in Fig. 1,
It has been found that there is a natural limit to the blocking ability, and although it is suitable for relatively low capacity devices, it is not suitable for high capacity devices.

このようなことから、大容量用の真空インタラプタとし
ては、歴史的には第1図に示す真空インタラプタよりも
早くから提案されている第2図に示すような真空インタ
ラプタ、すなわち縦磁界を発生するコイル8を真空容器
1の外部に配設してなる真空インタラプタの技術が見直
されてきた。
For this reason, as a vacuum interrupter for large capacity, the vacuum interrupter shown in Fig. 2, which has been proposed earlier than the vacuum interrupter shown in Fig. 1, has historically been proposed, that is, the coil that generates a longitudinal magnetic field. The technology of a vacuum interrupter in which a vacuum interrupter 8 is disposed outside the vacuum vessel 1 has been reviewed.

次に、第2図に示す真空インタラプタを説明するが第1
図と同一部材には同一符号を付して詳細な説明は省略す
る。
Next, the vacuum interrupter shown in FIG. 2 will be explained.
The same members as those in the figures are given the same reference numerals and detailed explanations will be omitted.

すなわち、各導電棒2a、2bの内端部には、それぞれ
II極3’tabのみが固着されている。
That is, only the II pole 3'tab is fixed to the inner end of each conductive rod 2a, 2b.

また真空容器1の外周部には、縦磁界を発生するコイル
8が巻回されており、このコイル8の一方の巻端側は、
接続リード9aを介して端子導体6&と接続され、また
他方の巻端側は接続リード9bを介して固定側の導電棒
2!Lと接続されている。
Further, a coil 8 that generates a vertical magnetic field is wound around the outer periphery of the vacuum container 1, and one winding end of this coil 8 is
It is connected to the terminal conductor 6& through the connection lead 9a, and the other end of the winding is connected to the fixed conductive rod 2 through the connection lead 9b! It is connected to L.

そして、このようtこ構成された真空インタラプタは、
絶縁フレームに収納されるとともに操作装置(ともに図
示省略)と接続されて真空しゃ断器として構成されてい
る。
The vacuum interrupter configured in this way is
It is housed in an insulating frame and connected to an operating device (both not shown) to form a vacuum breaker.

しかして、第2図に示す真空インタラプタは、次のよう
な利点がある。
The vacuum interrupter shown in FIG. 2 has the following advantages.

■ コイル8が真空容器1の外部に設けられているので
、コイル8に生ずるジュール熱を放散しやすい。
(2) Since the coil 8 is provided outside the vacuum vessel 1, Joule heat generated in the coil 8 can be easily dissipated.

■ コイル8が電極3a、3bとともに移動しないので
、アークに印加される縦磁界の強度変化がなく常に一定
である。
(2) Since the coil 8 does not move together with the electrodes 3a and 3b, the strength of the longitudinal magnetic field applied to the arc does not change and is always constant.

■ 可動部が軽量にしてかつ簡単な構造となる。■Movable parts are lightweight and have a simple structure.

しかしながら、第2図に示す真空インタラプタにあって
は、真空容器1の外周に配設されるコイル8の配置位置
およびコイル4の軸方向の長さ等の関係が不特定のため
、最適な強度の縦磁界を得ることができず、真空しゃ断
器の過度の大形化を招来している。
However, in the vacuum interrupter shown in FIG. 2, the relationship between the arrangement position of the coil 8 disposed on the outer periphery of the vacuum vessel 1 and the axial length of the coil 4 is unspecified, so that the optimum strength cannot be achieved. It is not possible to obtain a vertical magnetic field of 100 mm, resulting in an excessively large vacuum breaker.

本発明は、上述した問題に鑑みてなされたもので、その
目的とするところは、大きさをR適なものとし得る大容
量しゃ所用の真空しゃ断器を提供するにある。
The present invention has been made in view of the above-mentioned problems, and its purpose is to provide a vacuum breaker for large-capacity shutoff stations whose size is suitable for R.

この発明は、上記目的を達成するため、真空容器に1対
の導電棒を相対的に接近離反自在に導入するとともに、
各導電棒の内端部に′flL極をそれぞれ固着し、前記
真空容器の外周に導電棒の移動方向と同方向の磁界を発
生するコイルを配設してなる真空しゃ断器において、前
記コイルの軸方向の中心を、開極時の電極間中心に対し
軸方向へ:50ル萄の範囲内に位置せしめて設けること
により、アークに印加される縦磁界を最適な強度とする
ようにしたものである。
In order to achieve the above object, the present invention introduces a pair of conductive rods into a vacuum container so that they can approach and separate from each other, and
In a vacuum breaker, a 'flL pole is fixed to the inner end of each conductive rod, and a coil that generates a magnetic field in the same direction as the moving direction of the conductive rod is disposed around the outer periphery of the vacuum container. By locating the axial center within a range of 50 mm in the axial direction from the center between the electrodes when the electrode is opened, the longitudinal magnetic field applied to the arc is made to have the optimum strength. It is.

以下、第3図以降の図面を参照してこの発明の一実施例
を詳細に説明する。なお、以下の説明において第2図と
同一部材には同一符号を付して詳細な説明を省略する。
Hereinafter, one embodiment of the present invention will be described in detail with reference to the drawings from FIG. 3 onwards. In the following description, the same members as in FIG. 2 are denoted by the same reference numerals, and detailed description thereof will be omitted.

第3図は本発明の一実施例を示す真空しゃ断器の縦断面
図である。同図において10はエボキ樹脂等からなる有
底円筒状の絶縁フレームで、この絶縁フレーム■0には
、真空容器1の外周にコイル8を配設した真空インタラ
プタ11が、その可動側の導電棒2bを絶縁フレーム1
0の底部に設けた透孔12に挿通せしめて収納されてい
る。真空インタラプタ11のコイル8は、第4図に示す
ように、割譲状(約1ターン)のコイル部8aと、コイ
ル部8aの各端部から互いに平行にして軸方向および径
方向内方へ延在するL字形の第1.第2接続リード部8
b、 8cさ、第1.第2接続リード部8b。
FIG. 3 is a longitudinal sectional view of a vacuum breaker showing an embodiment of the present invention. In the same figure, reference numeral 10 denotes a bottomed cylindrical insulating frame made of epoxy resin, etc. In this insulating frame 0, a vacuum interrupter 11 having a coil 8 arranged around the outer periphery of the vacuum container 1 is mounted on a conductive rod on the movable side. 2b to insulation frame 1
It is housed by being inserted into a through hole 12 provided at the bottom of 0. As shown in FIG. 4, the coil 8 of the vacuum interrupter 11 includes a ceded coil portion 8a (approximately one turn) and a coil portion 8a extending in parallel to each other in the axial and radial directions from each end of the coil portion 8a. The L-shaped 1st. Second connection lead part 8
b, 8c, 1st. Second connection lead portion 8b.

8Cの端部に互いに径を異ならせて同心状に一体的に形
成された円筒状の第1 、f’g2コンタクトホルダ一
部8ct、3eとから構成されているとともに、第3図
に示すように、コイル部3aの軸方向の中心Pを、開極
時(しゃ断完了時)の電極間中心0と軸方向において同
位置に位置せしめて配設され、かつリングコンタクトま
たはマルチコンタクトの如き接触子13 、14を第1
コンタクトホルダ一部8dと可動側の導電棒2bとの間
および第2コンタクトホルダ一部8eと端子導体6N+
のコンタクトホルダ一部6′b′との間に介装すること
により、導電棒2bと端子導体6bとに電気的に接続さ
れている。
It consists of a cylindrical first contact holder part 8ct and part 3e having different diameters and integrally formed concentrically at the end of the contact holder 8C, and as shown in FIG. In this case, the axial center P of the coil portion 3a is located at the same position in the axial direction as the interelectrode center 0 at the time of opening (when the disconnection is completed), and a contactor such as a ring contact or a multi-contact is used. 13 and 14 as the first
Between the contact holder part 8d and the movable conductive rod 2b and between the second contact holder part 8e and the terminal conductor 6N+
The conductive rod 2b is electrically connected to the terminal conductor 6b by being interposed between the contact holder portion 6'b'.

なお、縦磁界印加によるしゃ断能力は、50g′ua/
に人のときが最高で、実用上40〜60gaus/にム
の範囲で実用上支障ないことが知られているが、コイル
8のコイル部8I!Lの軸方向の中心Pを開極時の電極
間中心C?+と軸方向において同位置とする場合は勿論
、コイル部8aの中心Pを開極時の電極間中心に対して
軸方向へ+ 5 Q m / mの範囲内に位置せしめ
て設けた場合にも、所望の磁界強度(4Q −5Q g
aus/′kA )を得ることができた。
In addition, the breaking ability by applying a vertical magnetic field is 50 g'ua/
It is known that there is no problem in practical use in the range of 40 to 60 gauss, but the coil part 8I of coil 8 is the highest when it is 200 gauss. Is the center P in the axial direction of L the center C between the electrodes when the electrodes are open? In addition to the case where the center P of the coil part 8a is located within the range of +5 Q m / m in the axial direction with respect to the center between the electrodes when the electrodes are opened, Also, the desired magnetic field strength (4Q −5Q g
aus/'kA).

また、コイル8のコイル部8aの中心Pを、上述した如
く電極間中心0と同位置とすれば、コイル部8aの幅り
は小さくても必要な縦磁界が得られるものの、このコイ
ル部81Llこより発生する磁界の磁力線はコイル部8
aの外形に沿って彎曲するので、アークに効果的な縦磁
界を印加するため、換言すればアークに印加される縦磁
界の磁力線を軸方向の平行なものとするため、コイル部
8aの軸方向の幅りを開極時の極間距離Gとほぼ等しく
設けである。
Further, if the center P of the coil portion 8a of the coil 8 is set at the same position as the interelectrode center 0 as described above, the necessary longitudinal magnetic field can be obtained even if the width of the coil portion 8a is small. The lines of magnetic force of the magnetic field generated from this are the coil part 8.
Since it is curved along the outer shape of the coil part 8a, in order to apply an effective vertical magnetic field to the arc, in other words, to make the lines of magnetic force of the vertical magnetic field applied to the arc parallel to the axial direction, the axis of the coil part 8a The width in the direction is set to be approximately equal to the distance G between the poles when the poles are opened.

さらに、コイル部8&が大径になると、これにより発生
する縦磁界の強度が、コイル部8aの中央部において低
下し、径方向に亘って均一な所要の磁界が得られなくな
るのを防止するため、コイル部8aの直径りを電極3a
、3bの直径dとの関係にセいてD/A≦2の関係を満
たすように設けである。
Furthermore, when the diameter of the coil portion 8& becomes large, the strength of the longitudinal magnetic field generated thereby decreases at the center of the coil portion 8a, and in order to prevent it from being impossible to obtain a uniform required magnetic field in the radial direction. , the diameter of the coil portion 8a is the electrode 3a.
, 3b so that the relationship D/A≦2 is satisfied.

以上の如く本発明によれば、真空容器の外周にし 配設されるコイルを最適な大きさのものとすることがで
きる等の効果を奏する。
As described above, according to the present invention, it is possible to make the coil disposed around the outer periphery of the vacuum container an optimal size.

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

@1図および繁2図はそれぞれ従来の真空インタラプタ
の縦断面図、第3図は本発明の一実施例を示′丁真空イ
ンタラプタの縦断面図、第4図は要部の分解斜視図であ
る。 1・・・真空容器、2a、21)・・・導電棒、3 a
 、3b・・・電極、8・・・コイル、O・・・電極間
中心、P・・・コイルの軸方向の中心。
Figures 1 and 2 are longitudinal cross-sectional views of a conventional vacuum interrupter, respectively. Figure 3 is a vertical cross-sectional view of a vacuum interrupter according to an embodiment of the present invention. Figure 4 is an exploded perspective view of the main parts. be. 1... Vacuum container, 2a, 21)... Conductive rod, 3 a
, 3b... Electrode, 8... Coil, O... Center between electrodes, P... Center in axial direction of coil.

Claims (1)

【特許請求の範囲】[Claims] 真空容器に1対の導電棒を相対的に接近兼自在に導入す
るとともに1各導電棒の内端部に電極をそれぞれ固着し
、前記真空容器の外周に導電棒の移動方向と同方向の磁
界を発生するコイルを配設してなる真空しゃ断器におい
て、前記コイルの軸方向の中心を、開極時の電極間中心
に対し軸方向へ±50 !1に/!+1の範囲内に位置
せしめて設けたことを特徴とする真空しゃ断器。
A pair of conductive rods are introduced into a vacuum container relatively close to each other and freely, electrodes are fixed to the inner ends of each conductive rod, and a magnetic field is applied to the outer periphery of the vacuum container in the same direction as the moving direction of the conductive rods. In a vacuum breaker, the axial center of the coil is set at an angle of ±50% in the axial direction from the center between the electrodes when the contacts are opened. To 1/! A vacuum breaker characterized in that it is located within a range of +1.
JP10449983A 1983-06-11 1983-06-11 Vacuum breaker Pending JPS59230226A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10449983A JPS59230226A (en) 1983-06-11 1983-06-11 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10449983A JPS59230226A (en) 1983-06-11 1983-06-11 Vacuum breaker

Publications (1)

Publication Number Publication Date
JPS59230226A true JPS59230226A (en) 1984-12-24

Family

ID=14382204

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10449983A Pending JPS59230226A (en) 1983-06-11 1983-06-11 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS59230226A (en)

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