JPS6185731A - Vacuum interrupter - Google Patents
Vacuum interrupterInfo
- Publication number
- JPS6185731A JPS6185731A JP20603984A JP20603984A JPS6185731A JP S6185731 A JPS6185731 A JP S6185731A JP 20603984 A JP20603984 A JP 20603984A JP 20603984 A JP20603984 A JP 20603984A JP S6185731 A JPS6185731 A JP S6185731A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- field generating
- electrode rod
- vacuum
- electrodes
- 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
Links
Landscapes
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
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
この発明は真空インタラプタに係り、特にアーりに対し
7て平行な軸方向の磁界を印加する、いわゆるfhIl
界印加方式の真空インタラプタに関する、従来の技術
従来、Eftla界印加方式の真空インタラプタとして
は例えば特開昭51−109480号公報に開示される
ものが知られている。この真空インタラプタは第4り1
に示すように、金属筒10両端にそれぞれ金属筒1と同
径の絶縁筒2a 、2bが固着されて筒体3が形成され
る。金属筒2a 、 2bの開口端は金属端&、 4
a 、 4 bで閉塞され、内部は高真空に排気されて
真空容器5が形成される。各金属端板4a、4bit真
空仰(真空容器4の内方)に突出されることにより大気
側に凹11s6a、6bが形成される。DETAILED DESCRIPTION OF THE INVENTION FIELD OF INDUSTRIAL APPLICATION This invention relates to a vacuum interrupter, and in particular to a so-called fhIl which applies an axial magnetic field parallel to the arc.
BACKGROUND OF THE INVENTION 2. Description of the Related Art Related to Field Application Vacuum Interrupters Conventionally, as an Eftla field application vacuum interrupter, one disclosed in Japanese Patent Application Laid-Open No. 109480/1983 is known. This vacuum interrupter is the fourth
As shown in FIG. 1, insulating cylinders 2a and 2b having the same diameter as the metal cylinder 1 are fixed to both ends of the metal cylinder 10, respectively, to form a cylinder 3. The open ends of the metal tubes 2a and 2b are metal ends &4
a and 4 b, and the inside is evacuated to a high vacuum to form a vacuum container 5. Recesses 11s6a and 6b are formed on the atmosphere side by protruding each metal end plate 4a to a 4-bit vacuum level (inside the vacuum container 4).
真空容器5内には、一方の全域端板4aから固定’m+
ii棒7が気密に導入さハており、他方の金属端板4b
から固定電極棒7に相対的に接近離反自在の可動X葎棒
8がベローズ9を介して気密に導入されている。ここに
、ベローズ9はその外方が高真空となるように真空容器
5内方に突出して設けらねている。固定電極棒7および
可動電極棒8の各内端部には対をなして接離自在の固定
電極10および可動電極11がそれぞれ固着されている
。また、固定電極棒7および可動電極棒8における電極
10 、31近傍には、シールド12 、13摂それぞ
れ取付けられている。前記各凹部5a 、5bには電極
10 、11と直列接続されたコイル状の磁界発生部材
14 、15が配設され、この磁界発生部材14 、1
5に電流1−流してアークと平行な磁界を発生させる。Inside the vacuum vessel 5, there are fixed 'm+
ii. The rod 7 is hermetically introduced, and the other metal end plate 4b
A movable X-shaft rod 8 which can be moved toward and away from the fixed electrode rod 7 is airtightly introduced through a bellows 9. Here, the bellows 9 is provided so as to protrude inside the vacuum container 5 so that the outside thereof is under high vacuum. A pair of fixed electrodes 10 and a movable electrode 11, which can be moved toward and away from each other, are fixed to the inner ends of the fixed electrode rod 7 and the movable electrode rod 8, respectively. Further, shields 12 and 13 are attached to the fixed electrode rod 7 and the movable electrode rod 8 near the electrodes 10 and 31, respectively. Coil-shaped magnetic field generating members 14 , 15 connected in series with electrodes 10 , 11 are disposed in each of the recesses 5 a , 5 b , and these magnetic field generating members 14 , 1
5 to generate a magnetic field parallel to the arc.
前記磁界発生部材14 、15と電極棒7,8との電気
的接続はイ)・・重子16 、17を介して行なわれる
。Electrical connection between the magnetic field generating members 14 and 15 and the electrode rods 7 and 8 is made via a) weights 16 and 17.
発明が%C決しようとする問題点
かη・る6成の真空インタラプタは電極背面に磁界発生
部材を設けたもののように構造が複雑で、しかも耐久性
が悪い等の欠点はない。また、真全容器の筒体外周に磁
界発生部材を設けたもののように真空インタラプタの大
型化および磁束密度確保のためのフィルターン数増加に
よる発熱等の問題もない。しかしながら、上記真空イン
タラプタにおいては、同定7I+極10と固定側の金属
端板4aとの間隔は非常に狭いのに対し、町動重、極1
1と可動側の金属端&4bとの間隔は広い。これはベロ
ーズ9の・トh方向長さが、一般°的に1イ極10 、
11の開極ILfにおける開極ギャップの4〜5倍程度
必要であり、そのベローズ9を真空容器5内方に突出さ
せて設けていることによる。このように、固定側と可動
側とが、電極10 、11の開極時に軸方向中心面に対
して非対称であると、電界分布の状態が不均一となって
耐電圧特性が非常に悪くなり、閃絡を惹起することにな
る。かかる電界分布の不均一による問題は高電圧になる
程顕著となる。Problems that the invention seeks to resolve The vacuum interrupter of the η·ru6 structure does not have the drawbacks of having a complicated structure and poor durability, unlike those in which a magnetic field generating member is provided on the back of the electrode. In addition, there are no problems such as heat generation due to an increase in the size of the vacuum interrupter and an increase in the number of filters to ensure magnetic flux density, unlike those in which a magnetic field generating member is provided on the outer periphery of the cylindrical body of a true container. However, in the above vacuum interrupter, the distance between the identification 7I+ pole 10 and the metal end plate 4a on the fixed side is very narrow;
The distance between 1 and the metal end &4b on the movable side is wide. This means that the length of the bellows 9 in the ・h direction is generally 1 pole 10,
This is because the bellows 9 is provided so as to protrude inward of the vacuum vessel 5. In this way, if the fixed side and the movable side are asymmetrical with respect to the axial center plane when the electrodes 10 and 11 are opened, the electric field distribution becomes uneven and the withstand voltage characteristics become very poor. , which will cause flashbacks. The problem caused by such non-uniform electric field distribution becomes more pronounced as the voltage becomes higher.
そこで、固定電離10と固定側の金属端板4aとの間隔
を広くして固定側と可動側とを対称形にすると、真空イ
ンタラプタが軸方向に大形化し、金属端板4&、4bの
凹部5a、5bに磁界発生部材14 、15を配設して
小形化を図った効果が没却されてしまう。また、磁界発
生部材14 、15間の距離が大きくなるとともに、電
極10 、11から磁界発生部材14 、15が離れる
ために磁界が有効に働かなくなってしゃ断性能が低下す
るという問題を生じる。Therefore, if the distance between the fixed ionization 10 and the metal end plate 4a on the fixed side is widened to make the fixed side and the movable side symmetrical, the vacuum interrupter becomes larger in the axial direction, and the recesses in the metal end plates 4&, 4b The effect of miniaturization by arranging the magnetic field generating members 14 and 15 at 5a and 5b is lost. Furthermore, as the distance between the magnetic field generating members 14 and 15 increases, the magnetic field generating members 14 and 15 are separated from the electrodes 10 and 11, causing the problem that the magnetic field no longer works effectively and the breaking performance deteriorates.
また、従来は磁界発生部材に全電流f流すものであった
。このためコイル長に比例して発熱が生じることから従
来の方式によって通電流の増加を図ることは困袴であっ
た。Furthermore, in the past, the entire current f was passed through the magnetic field generating member. For this reason, heat generation occurs in proportion to the coil length, making it difficult to increase the current flow using conventional methods.
問題点を解決するための手段
この発明は真空容器の両側板f71.空側に突出させて
大気俳に凹部を形成し、一方の凹部から容器内に固定電
極棒を導入し、他方の凹部からベローズを介して可動電
極≦くを導入し、両電極棒の端部にW極?設け、前記固
定電極棒の途中に所定の抵抜値を有する金JIJi部材
を介挿し、この金属部材の1i1ii端の1イ極棒に前
記一方の凹部に配設されるコイル状の61界発生部材t
m餓的に接続し、前言e他方の凹■〜の大気11+1に
磁性体を設けて構成したことにある。Means for Solving the Problems This invention provides two side plates f71. A concave portion is formed in the atmosphere by protruding toward the sky side, a fixed electrode rod is introduced into the container from one concave portion, a movable electrode is introduced from the other concave portion via a bellows, and the ends of both electrode rods are introduced into the container. W pole? A gold JIJi member having a predetermined resistance value is inserted in the middle of the fixed electrode rod, and a coil-shaped 61 field generation member is disposed in the one concave portion at one electrode rod at the 1i1ii end of this metal member. member t
The reason lies in the fact that they are connected in a continuous manner, and a magnetic material is provided in the atmosphere 11+1 of the other concave hole (1).
作用
上記のように真空インタラプタを構成し九ので、磁界発
生部材に流れる電流は固定電極棒に介挿された金属部材
の抵抗値により決定される。すなわち、分流されるので
磁界発生部材には全電流が流れない。このため、磁界発
生部材の発熱を抑制することができる。また、磁界発生
部材に流れる電流が少なくなるため、発生する磁束も低
減するが、これを補うために磁性体を設けて磁束が電極
側に集中させるよう圧する。Operation Since the vacuum interrupter is configured as described above, the current flowing through the magnetic field generating member is determined by the resistance value of the metal member inserted in the fixed electrode rod. That is, since the current is shunted, no current flows through the magnetic field generating member. Therefore, heat generation of the magnetic field generating member can be suppressed. Further, since the current flowing through the magnetic field generating member is reduced, the generated magnetic flux is also reduced, but in order to compensate for this, a magnetic body is provided to apply pressure so that the magnetic flux is concentrated on the electrode side.
実施例
以下図面を参照してこの発明を一実施例に基づき脱甲す
るに第4図と同一部分は同一符号を付して示す。Embodiment Hereinafter, referring to the drawings, the present invention will be explained based on one embodiment. The same parts as in FIG. 4 are designated by the same reference numerals.
第1図において、固定電極棒7は金属端板4aから気密
に導入される第1電極揮7aとこの第1重極、Nl 7
a K所定の抵抗値を有する金属部材20を介して連
結された第2電徐棒7bとから形成される。第1.第2
電橙搾7a、7bには凹部6aに収納されるコイル状の
磁界発生部材21が電気的に接続されている。すなわち
、磁界発生部材21は電気的に金属部材20と並列接続
された構成になる。In FIG. 1, a fixed electrode rod 7 includes a first electrode electrode 7a introduced airtightly from a metal end plate 4a, and this first heavy pole, Nl 7.
aK is formed from a second electric charge rod 7b connected via a metal member 20 having a predetermined resistance value. 1st. Second
A coil-shaped magnetic field generating member 21 housed in the recess 6a is electrically connected to the electric orange squeezers 7a and 7b. That is, the magnetic field generating member 21 is electrically connected to the metal member 20 in parallel.
なお、金属部材20の抵抗値は磁界発生部材2工の抵抗
値より多少大きいかあるいは略等しい値となるように予
め設定しておく。金属部材20は例えばFe系元素の単
体又は複炒の元素からなる合金のものである。Note that the resistance value of the metal member 20 is set in advance so as to be somewhat larger than or approximately equal to the resistance value of the two magnetic field generating members. The metal member 20 is made of, for example, an alloy of a single Fe-based element or a compound element.
可r#h電極棒8け凹部6bの大気側に配設したベロー
ズ22を介して金属端板4b1J−ら気密に導入される
。23はJU”:円板又はブロックからなる磁性体で、
この磁性体詔は可動側の凹s6bの電極背部位置に配設
させる。また、磁性体nは例えばFe系元素の単体又は
複数の元素からなる合金のものである。The eight electrode rods are introduced airtightly from the metal end plate 4b1J- through the bellows 22 disposed on the atmosphere side of the recess 6b. 23 is JU”: a magnetic material consisting of a disk or block,
This magnetic member is disposed at the back of the electrode in the recess s6b on the movable side. Further, the magnetic material n is, for example, a single Fe-based element or an alloy consisting of a plurality of elements.
上記のように真空インタラプタの固定電極棒7の途中に
所定の抵抗値を有する金属部材20を介挿して一部の電
流を、金属部材頷が持つ抵抗値と衿しいか、あるいけ小
さい抵抗値の磁界発生部材21に分流させて、磁界発生
部材21に全電流を流さないようにしたので、磁界発生
部材210発熱を抑制できる。また、可動W極11の背
後に磁性体23を配設したので、磁路が形成される。こ
のため、磁界発生部材21に流れる電流を金jri部材
20に流れる電流と略等しくしたときでも、磁性体23
により電極10 、11の部位に磁束を集中させること
ができるので、候磁界の作用によって伜れたしゃ断性能
が得られる。As described above, a metal member 20 having a predetermined resistance value is inserted in the middle of the fixed electrode rod 7 of the vacuum interrupter, and a part of the current is supplied to the fixed electrode rod 7 with a resistance value that is similar to or slightly smaller than the resistance value of the metal member. Since the current is shunted to the magnetic field generating member 21 so that the entire current does not flow through the magnetic field generating member 21, heat generation in the magnetic field generating member 210 can be suppressed. Furthermore, since the magnetic body 23 is disposed behind the movable W pole 11, a magnetic path is formed. Therefore, even when the current flowing through the magnetic field generating member 21 is made approximately equal to the current flowing through the metal member 20, the magnetic body 23
Since the magnetic flux can be concentrated at the electrodes 10 and 11, improved breaking performance can be obtained due to the action of the magnetic field.
第2図および第3図はこの発明の第2および第3実施例
を示すもので、43.2図は磁性体23を凹部6bの開
口面部に清って配トしたものであり、第3図は磁性体2
:つを凹部6bの側壁面に沿って配役するとともに磁性
体23の内側壁面に絶縁チューブ24 f if&けて
ベローズ22との接触を防止したものである。両実施例
とも上記と同様の作用効果がある。2 and 3 show the second and third embodiments of the present invention, and FIG. 43.2 shows the magnetic material 23 neatly arranged on the opening surface of the recess 6b; The figure shows magnetic material 2
The insulating tube 24 is placed along the side wall surface of the recess 6b, and an insulating tube 24 is placed on the inner wall surface of the magnetic body 23 to prevent contact with the bellows 22. Both embodiments have the same effects as above.
なお、上記実bjlI例においては、固定側のみに磁界
発生部材21を設けたが、本発明はかかる実施例に限定
式れるものではなく、磁界発生部材を可動側のみに設け
てもよく、また同定側および可動側の両方に設けてもよ
い。さらに、真空容器5の筒体は、金属筒10両端にそ
れぞれ絶縁筒2a、2bを固着したものの例で示したが
、筒体3全部が絶縁物で形成されるものでもよい。また
、筒体3は、その筒部が金属又は少なくとも両端が絶縁
物からなり、筒部両端に径方向内側の絶縁物からなる7
ランジを形成したものでもよい。In addition, in the above practical example, the magnetic field generating member 21 was provided only on the fixed side, but the present invention is not limited to such an embodiment, and the magnetic field generating member may be provided only on the movable side. It may be provided on both the identification side and the movable side. Furthermore, although the cylindrical body of the vacuum container 5 is shown as an example in which the insulating tubes 2a and 2b are fixed to both ends of the metal tube 10, the cylindrical body 3 may be entirely formed of an insulating material. Further, the cylinder 3 has a cylinder portion made of metal or at least both ends made of an insulating material, and a radially inner insulating material 7 at both ends of the cylinder portion.
A lunge may also be formed.
発明の効果
以上述べたように、この発明によれば、金属端板金真窒
側に突出させて大気僻に凹部を設けて真空容器を形成し
、その真空容器内部に電極を軸方向中心面が対称となる
ようにし、しかも可動筒、極の端板の大プ側にベローズ
及び磁性体を設けたので、電界分布が均一となカ耐電圧
の向上を図ることができる。また、この発明によれば、
磁性体を電極に接近させて配着でき磁界発生部材に約半
分のう流を流したことにより磁界の強さは半減するも1
F極間における磁束電度は全軍績をコイルに流した場合
と略同ζ・lにすることができ、上記の場合と相俟って
じゃ断性能が向上する。さらに、この発明によれは、磁
界発生部材に流れる電流が約半分になるので、磁界発生
部材の発熱を減少する。Effects of the Invention As described above, according to the present invention, a vacuum container is formed by providing a concave portion in the air with the metal end protruding toward the nitrogen side of the metal plate, and an electrode is placed inside the vacuum container so that the center surface in the axial direction Since the structure is symmetrical and the bellows and magnetic material are provided on the large side of the movable cylinder and the end plate of the pole, the electric field distribution is uniform and the withstand voltage can be improved. Further, according to this invention,
The strength of the magnetic field was halved by allowing the magnetic material to be placed close to the electrode and allowing approximately half of the flow to flow through the magnetic field generating member.
The magnetic flux electric power between the F poles can be made approximately the same ζ·l as when the entire force is passed through the coil, and together with the above case, the breaking performance is improved. Furthermore, according to the present invention, the current flowing through the magnetic field generating member is approximately halved, thereby reducing heat generation in the magnetic field generating member.
よって通t4々渾を増加させることができる。Therefore, it is possible to increase the throughput.
第1図はこの発明の一実施例を示す縦断面図、第2図お
よび第3図はこの発明の第2および第3実施例を示す縦
断1+図、テ、4図は従来例の真空インタラプタを示す
縦断面図である。
5・・・兵、空容器、5a、5b・・・凹部、7・・・
固定電極棒、8・・・可動市極棒、10・・・固定重積
、11・・・可動電極、20・・・金M部材、21・・
・磁界発生部材、22・・・ベローズ、23・・・磁性
体。FIG. 1 is a longitudinal sectional view showing one embodiment of the present invention, and FIGS. 2 and 3 are longitudinal sectional views 1+, TE, and 4 showing the second and third embodiments of the invention. FIG. 5... Soldier, empty container, 5a, 5b... recess, 7...
Fixed electrode bar, 8... Movable city pole bar, 10... Fixed stack, 11... Movable electrode, 20... Gold M member, 21...
- Magnetic field generating member, 22... bellows, 23... magnetic material.
Claims (1)
それぞれ金属端板で閉塞しかつ内部を高真空にするとと
もに、これら各金属端板を真空側に突出せしめることに
より大気側に凹部を設けて真空容器を形成し、この真空
容器内に一方の金属端板から固定電極棒を気密に導入し
、かつ他方の金属端板から固定電極棒に相対的に接近離
反自在の可動電極棒をベローズを介して気密に導入し、
これら両電極棒の各内端部に対をなして接離自在の電極
をそれぞれ設けてなる真空インタラプタにおいて、前記
電極の開極時に真空容器および電極を軸方向中心面に対
して対称となるように設けるとともに、前記凹部の少な
くとも一方に前記電極間に生じるアークと平行な磁界を
発生するコイル状の磁界発生部材を配設し、この磁界発
生部材が有する抵抗値より多少高いかあるいは低い抵抗
値を持つ金属部材を前記固定電極棒の通電路の途中に介
挿させて固定電極棒と磁界発生部材に通電電流を分流さ
せるように磁界発生部材を固定電極棒に接続し、前記ベ
ローズをその内方が高真空となるように可動側金属端板
の凹部に突出させるとともにその凹部の大気側に磁性体
を配設したことを特徴とする真空インタラプタ。(1) At least both ends of the cylindrical body are made of an insulator, and both ends are closed with metal end plates, the interior is made into a high vacuum, and each of these metal end plates is made to protrude toward the vacuum side, thereby creating a recess on the atmosphere side. A fixed electrode rod is airtightly introduced into the vacuum container from one metal end plate, and a movable electrode rod that can freely approach and separate from the fixed electrode rod is inserted from the other metal end plate into the vacuum container. Introduced airtight via bellows,
In a vacuum interrupter in which a pair of electrodes is provided at each inner end of each of these electrode rods, and the electrodes are movable toward and away from each other, the vacuum container and the electrodes are arranged symmetrically with respect to the axial center plane when the electrodes are opened. and a coil-shaped magnetic field generating member that generates a magnetic field parallel to the arc generated between the electrodes is disposed in at least one of the recesses, and the resistance value is slightly higher or lower than the resistance value of the magnetic field generating member. The magnetic field generating member is connected to the fixed electrode rod so that the conductive current is divided between the fixed electrode rod and the magnetic field generating member by inserting a metal member with a metal member in the middle of the current carrying path of the fixed electrode rod, and 1. A vacuum interrupter characterized in that the metal end plate on the movable side protrudes into a recess so as to create a high vacuum, and a magnetic material is disposed on the atmosphere side of the recess.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20603984A JPS6185731A (en) | 1984-10-01 | 1984-10-01 | Vacuum interrupter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20603984A JPS6185731A (en) | 1984-10-01 | 1984-10-01 | Vacuum interrupter |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6185731A true JPS6185731A (en) | 1986-05-01 |
Family
ID=16516879
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20603984A Pending JPS6185731A (en) | 1984-10-01 | 1984-10-01 | Vacuum interrupter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6185731A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014127280A (en) * | 2012-12-25 | 2014-07-07 | Toshiba Corp | Vacuum valve |
-
1984
- 1984-10-01 JP JP20603984A patent/JPS6185731A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014127280A (en) * | 2012-12-25 | 2014-07-07 | Toshiba Corp | Vacuum valve |
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