JP2892457B2 - Vacuum valve - Google Patents
Vacuum valveInfo
- Publication number
- JP2892457B2 JP2892457B2 JP2207498A JP20749890A JP2892457B2 JP 2892457 B2 JP2892457 B2 JP 2892457B2 JP 2207498 A JP2207498 A JP 2207498A JP 20749890 A JP20749890 A JP 20749890A JP 2892457 B2 JP2892457 B2 JP 2892457B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- magnetic field
- coil
- vacuum valve
- turn coil
- 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.)
- Expired - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H33/00—High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
- H01H33/60—Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
- H01H33/66—Vacuum switches
- H01H33/664—Contacts; Arc-extinguishing means, e.g. arcing rings
Landscapes
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
Description
【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、通電性能を低下させずに優れた遮断性能を
得る真空バルブに関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial application field) The present invention relates to a vacuum valve that obtains excellent shut-off performance without deteriorating energization performance.
(従来の技術) 真空バルブの遮断性能は、電極間に生じる磁界強度の
半径方向分布に依存し、この半径方向分布が平坦である
ほど遮断性能は優れる。(Prior Art) The shutoff performance of a vacuum valve depends on the radial distribution of the magnetic field strength generated between the electrodes, and the flatter the radial distribution, the better the shutoff performance.
従来の真空バルブは、電極の背面に設けるコイル電極
を軸方向磁界を発生する第1のコイルと第1のコイルが
発生させる軸方向磁界と相反する磁界を発生する第2の
コイルで構成し、これらの磁界を重ねあわせて電極中心
部の磁界強度を低下させて半径方向の磁界分布を平坦化
する。In a conventional vacuum valve, a coil electrode provided on the back surface of the electrode includes a first coil for generating an axial magnetic field, and a second coil for generating a magnetic field opposite to the axial magnetic field generated by the first coil. By superposing these magnetic fields, the magnetic field intensity at the center of the electrode is reduced, and the magnetic field distribution in the radial direction is flattened.
(発明が解決しようとする課題) 従来の真空バルブでは、コイル電極の電流通路が長く
なるため通電性能が低下し大容量化に不適であった。(Problems to be Solved by the Invention) In the conventional vacuum valve, the current path of the coil electrode becomes long, so that the current-carrying performance is deteriorated, which is not suitable for increasing the capacity.
本発明の目的は、計算での予測を可能にするとともに
通電性能を低下させずに遮断性能に優れた真空バルブを
提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a vacuum valve which enables prediction by calculation and which is excellent in shut-off performance without reducing current-carrying performance.
(課題を解決するための手段) 上記目的を達成するために本発明は、真空容器の内部
に接離自在に対向配置した固定電極および可動電極を有
し、これら両電極の背面に軸方向磁界を発生するコイル
電極を設けた真空バルブにおいて、両電極の背面にコイ
ル電極とは別に設けられ、コイル電極からの誘起電圧に
より磁界を発生し電極中心部の磁界を低減させるワンタ
ーンコイル電極を備えたことを要旨とする。(Means for Solving the Problems) In order to achieve the above object, the present invention has a fixed electrode and a movable electrode which are disposed in a vacuum vessel so as to be able to freely contact and separate from each other. In a vacuum valve provided with a coil electrode for generating a magnetic field, a one-turn coil electrode is provided on the back of both electrodes separately from the coil electrode and generates a magnetic field by an induced voltage from the coil electrode to reduce the magnetic field at the center of the electrode. That is the gist.
(作用) このような構成において、固定電極および可動電極の
背面とワンターンコイルを設け、コイル電極からの誘起
電圧により生じる磁界により予め計算により予測しワン
ターンコイルの形状を決定して両電極間に生じる半径方
向の磁界分布を平坦化するので、通電性能を低下させず
に遮断性能を向上することができる。(Operation) In such a configuration, the back surface of the fixed electrode and the movable electrode and a one-turn coil are provided, and the shape of the one-turn coil is determined by predicting in advance by a magnetic field generated by an induced voltage from the coil electrode, and is generated between the two electrodes. Since the magnetic field distribution in the radial direction is flattened, the breaking performance can be improved without lowering the current-carrying performance.
(実施例) 以下、本発明の実施例を図面を参照して説明する。(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.
第1図は本発明の真空バルブの電極部の断面図であ
る。なお、ここでは可動側を説明し固定側は省略する。FIG. 1 is a sectional view of an electrode portion of a vacuum valve of the present invention. Here, the movable side will be described and the fixed side will be omitted.
1は接点で2は電極であり、コイル電極5により誘起
されるうず電流が抑えられるようにスリットを充分に設
けておく。Reference numeral 1 denotes a contact and reference numeral 2 denotes an electrode, and a slit is sufficiently provided so that eddy current induced by the coil electrode 5 is suppressed.
3は接続子、4は補強部材であり、軸方向磁界を発生
するコイル電極5と電極2を接続するものである。な
お、接続子3は電極2のほぼ背面端部、補強部材4は電
極2のほぼ背面中央部に設けられている。Reference numeral 3 denotes a connector, and reference numeral 4 denotes a reinforcing member, which connects the coil electrode 5 for generating an axial magnetic field to the electrode 2. The connector 3 is provided substantially at the rear end of the electrode 2, and the reinforcing member 4 is provided substantially at the center of the rear of the electrode 2.
6は通電軸である。 Reference numeral 6 denotes an energizing shaft.
7はワンターンコイルで電極2の背面で且つ接続子
3、補強部材4の中間部に設けられ、電極を組み立てる
ときに電極ずれを防止するため、補強部材4とワンター
ンコイル7の内径との隙間をなくすようにしている。Reference numeral 7 denotes a one-turn coil which is provided on the back surface of the electrode 2 and at an intermediate portion between the connector 3 and the reinforcing member 4, and prevents a gap between the reinforcing member 4 and the inner diameter of the one-turn coil 7 in order to prevent electrode displacement when assembling the electrode. I'm trying to get rid of it.
次に本発明の作用について説明する。 Next, the operation of the present invention will be described.
接点1及び電極2にスリットを設けてあるのでコイル
電極5により電極間に発生する磁界を計算することが可
能である。次に、ワンターンコイル電極7に流れるうず
電流を求める。ワンターンコイル電極7に流れるうず電
流を求めるにはまずワンターンコイル電極7とコイル電
極5の発生する磁界との磁束鎖交数を計算する必要があ
り次式により計算ができる。Since the contact 1 and the electrode 2 are provided with slits, the magnetic field generated between the electrodes by the coil electrode 5 can be calculated. Next, an eddy current flowing through the one-turn coil electrode 7 is obtained. In order to obtain the eddy current flowing through the one-turn coil electrode 7, first, it is necessary to calculate the number of magnetic flux linkages between the one-turn coil electrode 7 and the magnetic field generated by the coil electrode 5, which can be calculated by the following equation.
φ(磁束鎖交数)=∫sBds…(1)(記号:第2図参
照) 又、ワンターンコイルに誘起される電圧υは次式で求
められる。φ (number of magnetic flux linkages) = ∫ s Bds (1) (symbol: see FIG. 2) Further, the voltage に induced in the one-turn coil can be obtained by the following equation.
ここで、第2図はワンターンコイル7の拡大図であ
り、このA−A断面図である第3図のBはコイル電極5
により発生する磁界、Sはワンターンコイル7で囲まれ
る領域、Aはワンターンコイル7の断面積である。なお
(1)式および(2)式のB,Sはこれを採用した。 Here, FIG. 2 is an enlarged view of the one-turn coil 7, and FIG.
, S is a region surrounded by the one-turn coil 7, and A is a cross-sectional area of the one-turn coil 7. This is adopted for B and S in the equations (1) and (2).
従って、ワンターンコイル電極に流れるうず電流iは
次式の微分方程式を解くことによって求められる。Therefore, the eddy current i flowing through the one-turn coil electrode can be obtained by solving the following differential equation.
ここでLはワンターンコイル7のインダクタンス、R
はワンターンコイル7の抵抗でR=ρ×2πr/Aで求ま
りρは低効率である。 Here, L is the inductance of the one-turn coil 7, R
Is the resistance of the one-turn coil 7 and is determined by R = ρ × 2πr / A, and ρ is low efficiency.
以上のように、ワンターンコイル電極7に流れるうず
電流を計算で容易に求めることができるので、ワンター
ンコイル電極7に流れるうず電流による磁界が計算でき
る。この結果とコイル電極5による磁界の計算結果を重
ね合わせることにより実際の磁界分布を求めることがで
きる。従って第4図の磁界分布図のように、従来のAで
ある特性からBのようなフラットな特性となるようにワ
ンターンコイル7の形状を調整する。As described above, since the eddy current flowing through the one-turn coil electrode 7 can be easily obtained by calculation, the magnetic field due to the eddy current flowing through the one-turn coil electrode 7 can be calculated. The actual magnetic field distribution can be obtained by superimposing this result and the calculation result of the magnetic field by the coil electrode 5. Therefore, as shown in the magnetic field distribution diagram of FIG. 4, the shape of the one-turn coil 7 is adjusted so that the conventional characteristic of A becomes a flat characteristic such as B.
このように本発明は電極の背面にコイル電極からの磁
界に誘起されるうず電流を流すワンターンコイルを設
け、計算で求まるうず電流を流す場所およびうず電流値
となるようにワンターンコイルの形状を調整するので、
電極間の半径方向の磁界強度分布を平坦化することがで
き、通電性能を低下させずに遮断性能を向上することが
できる。As described above, according to the present invention, a one-turn coil for passing an eddy current induced by a magnetic field from the coil electrode is provided on the back surface of the electrode, and the shape of the one-turn coil is adjusted so that the eddy current value and the location where the eddy current is obtained by calculation are obtained. So
The magnetic field strength distribution in the radial direction between the electrodes can be flattened, and the cutoff performance can be improved without lowering the conduction performance.
第1図は本発明の真空バルブの電極部の断面図、第2図
はワンターンコイルの拡大図、第3図は第2図のA−A
断面図、第4図は電極間の半径方向の磁界分布図であ
る。 2……電極、5……コイル電極 7……ワンターンコイルFIG. 1 is a sectional view of an electrode portion of a vacuum valve of the present invention, FIG. 2 is an enlarged view of a one-turn coil, and FIG.
FIG. 4 is a sectional view of the magnetic field distribution between the electrodes in the radial direction. 2 ... electrode 5 ... coil electrode 7 ... one-turn coil
Claims (1)
固定電極および可動電極を有し、これら両電極の背面に
軸方向磁界を発生するコイル電極を設けた真空バルブに
おいて、 前記両電極の背面に前記コイル電極とは別に設けられ、
前記コイル電極からの誘起電圧により磁界を発生し電極
中心部の磁界を低減させるワンターンコイル電極を備え
たことを特徴とする真空バルブ。1. A vacuum valve having a fixed electrode and a movable electrode which are arranged inside and inside a vacuum vessel so as to be able to freely contact with and separate from each other, and a coil electrode for generating an axial magnetic field on the back of both electrodes. Is provided separately from the coil electrode on the back of
A vacuum valve comprising a one-turn coil electrode for generating a magnetic field by an induced voltage from the coil electrode and reducing a magnetic field at the center of the electrode.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2207498A JP2892457B2 (en) | 1990-08-07 | 1990-08-07 | Vacuum valve |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2207498A JP2892457B2 (en) | 1990-08-07 | 1990-08-07 | Vacuum valve |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0492328A JPH0492328A (en) | 1992-03-25 |
| JP2892457B2 true JP2892457B2 (en) | 1999-05-17 |
Family
ID=16540711
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2207498A Expired - Lifetime JP2892457B2 (en) | 1990-08-07 | 1990-08-07 | Vacuum valve |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2892457B2 (en) |
-
1990
- 1990-08-07 JP JP2207498A patent/JP2892457B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0492328A (en) | 1992-03-25 |
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