JPS5828122A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS5828122A
JPS5828122A JP12729381A JP12729381A JPS5828122A JP S5828122 A JPS5828122 A JP S5828122A JP 12729381 A JP12729381 A JP 12729381A JP 12729381 A JP12729381 A JP 12729381A JP S5828122 A JPS5828122 A JP S5828122A
Authority
JP
Japan
Prior art keywords
electrode
magnetic field
outer diameter
coil
vacuum
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.)
Granted
Application number
JP12729381A
Other languages
Japanese (ja)
Other versions
JPS6338807B2 (en
Inventor
泰司 野田
佐野 孝光
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 JP12729381A priority Critical patent/JPS5828122A/en
Publication of JPS5828122A publication Critical patent/JPS5828122A/en
Publication of JPS6338807B2 publication Critical patent/JPS6338807B2/ja
Granted legal-status Critical Current

Links

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】 部に電棲面と直交する軸方向磁界を発住させるコイルを
配設してなる真孕しゃ断4に関する。
DETAILED DESCRIPTION OF THE INVENTION This invention relates to a true breaker 4 in which a coil for generating an axial magnetic field perpendicular to the electrostatic surface is disposed.

一般に、真突しゃ断器は,第1図に示すよう薔こ。Generally, a straight-on breaker has a rose-shaped structure as shown in Figure 1.

円筒状に形威したガラスまたはセラミックからなる絶縁
筒1の両端を円板状の金属端板2にまりタ密に閉塞して
真空容漏3を形成するとともに,この真空容器3内に1
対の電極4を両金属端板2の中央部から相対的に接近離
反自在に導入した対をなす電極棒5を介し接触離反(側
1自在に設けて構成されている。
Both ends of a cylindrical insulating cylinder 1 made of glass or ceramic are tightly closed by a disc-shaped metal end plate 2 to form a vacuum leak 3, and a vacuum chamber 3 is formed inside the vacuum vessel 3.
A pair of electrodes 4 are introduced from the center portions of both metal end plates 2 so as to be able to approach and separate from each other via a pair of electrode rods 5, so that they can come into contact with each other and move away from each other (sides 1 can be moved freely).

しかし、一般的な真空しゃ断器においてしゃ断時に発生
するアークは、それ自身の磁界と外部回路の磁界の相互
作用により著しく不安定となり。
However, the arc that occurs when a typical vacuum breaker breaks is extremely unstable due to the interaction between its own magnetic field and the magnetic field of the external circuit.

電極面を移動するとともにその周辺部に偏在し。As it moves along the electrode surface, it is unevenly distributed around the electrode surface.

電極を局部的に加熱して多量の金属蒸気を放出し、結果
的にしゃ断容量の低下を招来している。
The electrode is locally heated and a large amount of metal vapor is emitted, resulting in a decrease in interrupting capacity.

かかる問題に対処するため,第2図に示すようlこ、電
極4の背部に、電極棒5に流れる電流を電極棒5を史心
とするループ電流に変喚して電極面と直交する軸方向(
第2図において上下方向)磁界を発生させるコイル6を
配役し、コイル6から発生する軸方向磁界によりアーク
を電極面に均一に拡散してしゃ断容量を高めるようにし
た。いわゆる縦磁界電極の真空しゃ断器が知られている
In order to deal with this problem, as shown in FIG. 2, a current flowing through the electrode rod 5 is transformed into a loop current with the electrode rod 5 as the center of the current, and an axis perpendicular to the electrode surface is installed on the back of the electrode 4. direction(
A coil 6 that generates a magnetic field (in the vertical direction in FIG. 2) is provided, and the axial magnetic field generated by the coil 6 uniformly diffuses the arc over the electrode surface to increase the breaking capacity. A so-called vertical magnetic field electrode vacuum breaker is known.

ところが、縦磁界電極の真空しゃ断器においては、コイ
ル6によって発生する軸方向磁界が、通常鋼からなる電
極II5とgl交することにより電極4!115にうず
電流が生じ、このうず電流によって生ずる磁界が軸方向
磁界を低減するように作用するので、その分だけしゃ断
容量の低下をもたらしている。
However, in a vacuum breaker with vertical magnetic field electrodes, the axial magnetic field generated by the coil 6 intersects with the electrode II5 made of normal steel, causing eddy currents in the electrodes 4!115, and the magnetic field generated by this eddy current acts to reduce the axial magnetic field, resulting in a corresponding reduction in the breaking capacity.

本発明は上述した間部に鑑みてなされたもので。The present invention has been made in view of the above-mentioned problems.

その目的とするところは、電極棒の形状等を改良するこ
とにより、電極棒に生ずるうず電流の低下を図り、もっ
てコイルによって発生する軸方向磁界の損失を低減し、
ひいては効果的にしゃ断容量を高め得るようにした縦磁
界電極の真空しゃ断器を楊供するにある。
The purpose of this is to reduce the eddy current generated in the electrode rod by improving the shape etc. of the electrode rod, thereby reducing the loss of the axial magnetic field generated by the coil.
Another object of the present invention is to provide a vacuum breaker with vertical magnetic field electrodes that can effectively increase the breaking capacity.

以下、第3図以降の図面を参照してこの発明の実施例を
群細に説明する。なお−以下の説明において前述したも
のの構成部材と同一機能を奏する構成部材にはト1−符
号を付し重書する説明を4i略する。
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings from FIG. 3 onwards. In the following description, structural members that have the same functions as those described above are designated by the reference numerals 1 and 4i, and overlapping descriptions will be omitted.

第3図は本発明に係る真空しゃ断器の要部の断面図で、
真空容N(図示′4i略)内に相対的に接近離反自在に
導入される鋼からなる1対の電極棒5の内端部には、所
定の長さに亘って小径部51が形成されている。小径部
5aは、コイル6によって発生する軸方向磁界の@交を
低減して、うず電流が電極棒54こ発生するのを減少せ
しめるためのもので、コイル6の中間部と対応する電極
棒5の内端(#3図において上端)から電極4の外径り
のζ以上の長さLに相当する部分の外径dを30rm以
下として形成されており、この小径部5a番こは機械的
強度を高めて高電圧の電流の投入、しゃ断を可能にすべ
くステンレス鋼からなる補強パイプ1がろう付は等によ
り嵌着されている。
FIG. 3 is a sectional view of the main parts of the vacuum breaker according to the present invention,
A small diameter portion 51 is formed over a predetermined length at the inner end portions of a pair of electrode rods 5 made of steel that are introduced into a vacuum volume N (not shown in the figure '4i) so as to be able to approach and separate from each other. ing. The small diameter portion 5a is for reducing the cross-over of the axial magnetic field generated by the coil 6 to reduce the generation of eddy current on the electrode rod 54. The outer diameter d of the portion corresponding to the length L of the outer diameter of the electrode 4 from the inner end (upper end in figure #3) of ζ or more is 30 rm or less, and this small diameter portion 5a is mechanically A reinforcing pipe 1 made of stainless steel is fitted by brazing or the like in order to increase the strength and enable high-voltage current to be turned on and off.

なお、小径部5aは、電極棒5の外径が30m1mを超
えた場合に形成されるもので、電極棒5の外径が全長に
亘って30 m/m以下の場合に形成されないのは勿論
である。また、補強バイブ7は、その円周面と小径部5
aの外周面とが密着していても、両面間に7I!隙があ
っても差し支えがないものである。
Note that the small diameter portion 5a is formed when the outer diameter of the electrode rod 5 exceeds 30 m/m, and of course is not formed when the outer diameter of the electrode rod 5 is 30 m/m or less over the entire length. It is. Further, the reinforcing vibrator 7 has a circumferential surface and a small diameter portion 5.
Even if the outer peripheral surface of a is in close contact, there is 7I between both surfaces! There is no problem even if there are gaps.

ここで、電極棒5の外径の変化および外温変化の範囲(
長さ)の変化によってうず電流が発生する割合、換言す
れば電極II5の形状変化によってコイル6から発生す
る軸方向磁界が受ける影響は。
Here, the range of change in the outer diameter of the electrode rod 5 and change in external temperature (
In other words, the rate at which eddy current is generated due to a change in the length of the electrode II5, or in other words, the effect that the axial magnetic field generated from the coil 6 is affected by a change in the shape of the electrode II5.

第4図に示す実験結果のようになった。すなわち、第4
図は、横軸に電極@Sの外径を、また縦軸に電極棒5が
ない場合を100%とする電極面中心部の磁束密度をと
ったもので、その曲線Aは電極棒5の外径を全長に亘っ
て一様に変化させたもの。
The experimental results are as shown in FIG. That is, the fourth
In the figure, the horizontal axis represents the outer diameter of the electrode @S, and the vertical axis represents the magnetic flux density at the center of the electrode surface with the case where there is no electrode rod 5 as 100%. The outer diameter changes uniformly over the entire length.

曲線Bは電極棒5の外径変化の範囲をW接極りのζ以上
としたもの、曲線Cは電極棒5の外径変化の範囲を電極
りのζ以上としたもの、また曲dpは電極l1I5の外
径変化の範囲を電極径り以上としたものをそれぞれ示し
ている。したがって−電極棒5の内端部における電極径
りの14以上の長さに相当する範囲の部分の外径を30
 rrvm以1とすることにより、うず電流による影響
を4011以下に低減できることが判る。
Curve B is a curve in which the range of change in the outer diameter of the electrode rod 5 is greater than ζ of the W armature, curve C is a curve in which the range of change in the outer diameter of the electrode bar 5 is greater than ζ of the electrode, and curve dp is The range of change in the outer diameter of the electrodes I1I5 is shown to be greater than or equal to the electrode diameter. Therefore, the outer diameter of the area corresponding to a length of 14 or more of the electrode diameter at the inner end of the electrode rod 5 is 30
It can be seen that by setting rrvm to 1, the influence of eddy current can be reduced to 4011 or less.

以上の如く本発明は、真空容器内に1対の電極を相対的
に接近離反自在に導入した対をなす電極棒を介し接離自
在に設けるとともに、各電極の背部に軸方向磁界を発生
させるコイルを配設してなる真空しゃ断5+こおいて、
前配各電極柳におけるそれぞれのコイルの中間部から電
極の外径権以上の長さに相当する部分の外径を30Vm
以下としたものであるから、軸方向磁界の′ぽ極欅に対
する鎖交が低減されるので、うず電流の発生を大幅に低
減できる。したがって、軸方向磁界を電極面に有効に作
用せしめることができ、縦磁界電極の真空しゃ断器のし
ゃ断容量を効果的に高めることができる等の効果を奏す
る。
As described above, the present invention provides a pair of electrodes in a vacuum container so as to be able to move toward and away from each other via a pair of electrode rods that are introduced into a vacuum container so as to be able to approach and move away from each other, and to generate an axial magnetic field at the back of each electrode. A vacuum cutoff 5+ formed by arranging a coil,
The outer diameter of the part corresponding to the length from the middle part of each coil of each front electrode to the outer diameter of the electrode is 30Vm.
Since it is as follows, the linkage of the axial magnetic field to the 'polar key' is reduced, so that the generation of eddy current can be significantly reduced. Therefore, the axial magnetic field can be effectively applied to the electrode surface, and the breaking capacity of the vacuum breaker of the vertical magnetic field electrode can be effectively increased.

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

第1図は一般的な真9しゃ断器の概略fl152図。 第2図は縦磁界電極の概略説明図、第3図は本発明に係
る真空しゃ断器の要部断面図、84図は本発明に係る電
極棒の形状変化ζこよって蛍ける軸方向磁界の影響の実
験結果を表わした説明図である。 3・・・真空容器、4・・・電極、6・・・電極棒、5
h・・・小径部、6・・・コイル。 第1図 第2図 第4図 tオケネFつ外径 第3図
Figure 1 is a schematic fl152 diagram of a general true 9 circuit breaker. Fig. 2 is a schematic explanatory diagram of a vertical magnetic field electrode, Fig. 3 is a sectional view of a main part of a vacuum breaker according to the present invention, and Fig. 84 is a diagram illustrating the change in shape of the electrode rod according to the present invention. It is an explanatory diagram showing the experimental results of influence. 3... Vacuum container, 4... Electrode, 6... Electrode rod, 5
h...Small diameter part, 6...Coil. Figure 1 Figure 2 Figure 4 Figure 3 Outer diameter Figure 3

Claims (1)

【特許請求の範囲】[Claims] 真空容4内に1対の電極を相対的に接近離反自在に導入
した対をなす電極棒を介し接離自在に設けるとともに、
各電極の背部に軸方向磁界を発生させるコイルを配設し
てなる真空しゃ断器において、前記各電極棒におけるそ
れぞれのコイルの中間部から電極の外径−以上の長さに
相当する部分の外径)) 30 m / m以下とした
ことを特徴とする真空しゃ断器。
A pair of electrodes are introduced into the vacuum volume 4 so as to be able to approach and separate from each other via a pair of electrode rods, and
In a vacuum breaker in which a coil for generating an axial magnetic field is disposed on the back of each electrode, a portion of the electrode rod extending from the middle of each coil to a length corresponding to the outer diameter of the electrode or more. A vacuum breaker characterized in that the diameter is 30 m/m or less.
JP12729381A 1981-08-13 1981-08-13 Vacuum breaker Granted JPS5828122A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12729381A JPS5828122A (en) 1981-08-13 1981-08-13 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12729381A JPS5828122A (en) 1981-08-13 1981-08-13 Vacuum breaker

Publications (2)

Publication Number Publication Date
JPS5828122A true JPS5828122A (en) 1983-02-19
JPS6338807B2 JPS6338807B2 (en) 1988-08-02

Family

ID=14956373

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12729381A Granted JPS5828122A (en) 1981-08-13 1981-08-13 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS5828122A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11811373B2 (en) 2018-12-19 2023-11-07 Mitsubishi Electric Corporation Class AB amplifier and operational amplifier

Also Published As

Publication number Publication date
JPS6338807B2 (en) 1988-08-02

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