JPH03246840A - Vacuum valve - Google Patents

Vacuum valve

Info

Publication number
JPH03246840A
JPH03246840A JP4128290A JP4128290A JPH03246840A JP H03246840 A JPH03246840 A JP H03246840A JP 4128290 A JP4128290 A JP 4128290A JP 4128290 A JP4128290 A JP 4128290A JP H03246840 A JPH03246840 A JP H03246840A
Authority
JP
Japan
Prior art keywords
current
electrode
reinforcing member
coil electrode
resistance value
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
JP4128290A
Other languages
Japanese (ja)
Inventor
Kenji Watanabe
憲治 渡辺
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 JP4128290A priority Critical patent/JPH03246840A/en
Publication of JPH03246840A publication Critical patent/JPH03246840A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H33/00High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
    • H01H33/60Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
    • H01H33/66Vacuum switches
    • H01H33/664Contacts; Arc-extinguishing means, e.g. arcing rings

Abstract

PURPOSE:To reduce the power loss at the time of excitation by providing a reinforcing member connected to an exciting shaft and inserted into a coil electrode and having a positive resistance temperature coefficient between the exciting shaft and the back face of an electrode. CONSTITUTION:A reinforcing member 6 connected to an exciting shaft 5 and inserting into a coil electrode 4 and having a positive resistance temperature coefficient is provided between the exciting shaft 5 and the back face of an electrode 1. The reinforcing member 6 arranged between the back face of the electrode 1 and the exciting shaft 5 prevents the deformation of the electrode 1 and the coil electrode 4, the reinforcing member 6 has a high resistance value due to the cutoff current at the time of a cutoff, thus a current flows in the coil electrode 4, and a current flows in the reinforcing member 6 having a low resistance value at the time of excitation. The power loss on the current path of the coil electrode 4 at the time of excitation can be reduced.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は通電時(閉極時)における電力損失を低減でき
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 can reduce power loss when energized (closed).

(従来の技術) 一般に大電流遮断用の真空バルブは、電極間に軸方向磁
界を発生する縦磁界電極構造である。
(Prior Art) Vacuum valves for interrupting large currents generally have a vertical magnetic field electrode structure that generates an axial magnetic field between electrodes.

この縦磁界電極は電流遮断時に軸方向磁界により、アー
クが電極間に均一に分散されてアークの集中及び電極の
溶融を防ぎ遮断性能を向上させるものである。また、電
極と通電軸間の補強部材はステンレスを使用している。
This vertical magnetic field electrode uses an axial magnetic field to disperse the arc uniformly between the electrodes during current interruption, thereby preventing concentration of the arc and melting of the electrode, thereby improving the interruption performance. Furthermore, the reinforcing member between the electrode and the current-carrying shaft is made of stainless steel.

(発明が解決しようとする課題) 上述のような真空バルブの縦磁界電極構造は、補強部材
の抵抗値が大きいため通電時および遮断時の電流は常に
コイル電極を流れる。またコイル電極の電流路は長いの
でコイル電極の抵抗値は大きい。従って大電流通電にお
いては電力損失が大きくなるという問題点があった。
(Problems to be Solved by the Invention) In the vertical magnetic field electrode structure of the vacuum valve as described above, since the reinforcing member has a large resistance value, current always flows through the coil electrode during energization and energization. Furthermore, since the current path of the coil electrode is long, the resistance value of the coil electrode is large. Therefore, there is a problem in that power loss increases when a large current is applied.

本発明の目的は、遮断性能を低下させずに通電時(閉極
時)の電力損失を低減できる真空バルブを提供すること
にある。
An object of the present invention is to provide a vacuum valve that can reduce power loss during energization (when closed) without reducing the interrupting performance.

〔発明の構成〕[Structure of the invention]

(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、真空容器内に接離
自在に設けられ通電軸に取付けられた1対の電極の少な
くとも一方の背面に通電軸から接続されるコイル電極を
有する真空バルブにおいて、通電軸と電極背面間に通電
軸に接続され且つコイル電極に嵌入されて設けられる正
の抵抗温度係数を有する補強部材で構成する。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides a connection from the current-carrying shaft to the back surface of at least one of a pair of electrodes that are provided in a vacuum container so as to be able to come and go and are attached to the current-carrying shaft. In a vacuum valve having a coil electrode, the reinforcing member has a positive temperature coefficient of resistance and is connected to the current-carrying shaft and fitted into the coil electrode between the current-carrying shaft and the back surface of the electrode.

(作用) 電極背面と通電軸間の補強部材は、電極とコイル電極の
変形を防止するとともに通電時は低紙:抗で遮断時の遮
断電流により高抵抗になりコイル電極に遮断電流が流れ
るため、遮断性能を低下させることなく通電時の電力損
失を低減できる。
(Function) The reinforcing member between the back of the electrode and the current-carrying shaft prevents deformation of the electrode and coil electrode, and when energized, the reinforcement member has a low resistance when energized, so the breaking current at the time of interruption becomes high resistance, and the breaking current flows to the coil electrode. , it is possible to reduce power loss during energization without reducing interrupting 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) Embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明による真空バルブの電極の断面図である
FIG. 1 is a sectional view of an electrode of a vacuum valve according to the invention.

図の下側は可動側、上側は固定側を示す。The lower side of the figure shows the movable side, and the upper side shows the fixed side.

lは電極で、接点2が電極10表面に固定される。1 is an electrode, and a contact point 2 is fixed to the surface of the electrode 10.

3は接続子で接点2とは反対側の電極1の裏面に固定さ
れる。
A connector 3 is fixed to the back surface of the electrode 1 on the opposite side from the contact 2.

4はコイル電極で、通電軸5から放射状に伸びる図示し
ない複数個の腕部とこれら各腕部の突出端に向は且つ先
端が隣りあう腕部の突出端に対して適宜の間隙を存する
ように同一方向の円弧を描かせたコイル部から成り、接
続子3を介して電極1に接続される。
Reference numeral 4 denotes a coil electrode, which has a plurality of arm portions (not shown) extending radially from the current-carrying shaft 5, and the protruding ends of each of these arm portions are directed toward each other, and the tips thereof are arranged with appropriate gaps between the protruding ends of the adjacent arm portions. It consists of a coil portion drawn in circular arcs in the same direction, and is connected to the electrode 1 via a connector 3.

主として電流遮断時に縦方向(軸方向)磁界を発生して
アークを電極間に均一に分散してアークの集中及び電極
の溶融を防止する。また対向する固定側電極のコイル電
極も同様な構造にして電極間には均一な磁界が発生する
Mainly when the current is cut off, a longitudinal (axial) magnetic field is generated to uniformly disperse the arc between the electrodes, thereby preventing concentration of the arc and melting of the electrodes. Further, the coil electrodes of the opposing fixed side electrodes have a similar structure so that a uniform magnetic field is generated between the electrodes.

6は補強部材で、電極の開閉時に加わる外方により電極
1とコイル電極4の変形を防止する。
A reinforcing member 6 prevents deformation of the electrode 1 and the coil electrode 4 due to external force applied when the electrodes are opened and closed.

そのため、接続する通電軸5の上部とともにコイル電極
4の挿入穴にはめこんでロウ付けされ、且つ電極1に接
続される。電流通電時には補強部材6に、電流遮断時に
はコイル電極4がアークを均一に分散するのに十分な磁
界を発生させるためコイル電極4に電流が流れるように
補強部材6の材質を選定する。例えばV2O3セラミ、
りのような正の抵抗温度係数をもつ特性(PTC特性)
の材料を使用すれば、電流通電時は低抵抗なので補強部
材6に、電流遮断時は高抵抗になるのでコイル電極4に
電流が流れる。このように通電時から遮断時において十
分な抵抗変化が得られるので、単に抵抗値を大きくする
ための円筒形にする必要はなく円柱形で構わない。
Therefore, it is fitted into the insertion hole of the coil electrode 4 together with the upper part of the energizing shaft 5 to be connected and brazed, and is connected to the electrode 1. The material of the reinforcing member 6 is selected so that the current flows through the reinforcing member 6 when the current is applied and the coil electrode 4 generates a magnetic field sufficient to uniformly disperse the arc when the current is interrupted. For example, V2O3 ceramic,
Characteristics with a positive temperature coefficient of resistance (PTC characteristics) such as
If this material is used, current will flow to the reinforcing member 6 because it has low resistance when current is applied, and to the coil electrode 4 because it has high resistance when current is interrupted. In this way, a sufficient change in resistance can be obtained from the time of energization to the time of energization, so it is not necessary to use a cylindrical shape simply to increase the resistance value, but a cylindrical shape may be used.

次にこの真空パル、プの作用を第2図を参照して説明す
る。
Next, the action of this vacuum pulse will be explained with reference to FIG.

第2図は補強部材6をv203セラミックとした場合の
通電電流に対する抵抗値の変化を示す特性である。定格
通電電流値irc付近では補強部材6の抵抗値は約0.
5〔μg〕で、これはコイル電極4の抵抗値より十分に
小さい。従って通電時の電流はほとんど補強部材6を流
れるので、コイル電極4の電力損失は小さくなり電流流
路の長さの影響はほとんど受けなくなる。また、補強部
材6を流れる電流による発熱分及び通電時(閉極時)の
接触抵抗による発熱分は、補強部材6を円柱状にしたた
め熱伝導によって熱を取り去ることができる。
FIG. 2 shows the characteristics showing the change in resistance value with respect to the applied current when the reinforcing member 6 is made of V203 ceramic. The resistance value of the reinforcing member 6 is approximately 0.0 at around the rated current value IRC.
5 [μg], which is sufficiently smaller than the resistance value of the coil electrode 4. Therefore, most of the current when energized flows through the reinforcing member 6, so that the power loss of the coil electrode 4 is small and is almost unaffected by the length of the current flow path. In addition, heat generated by the current flowing through the reinforcing member 6 and heat generated by contact resistance during energization (when closed) can be removed by heat conduction because the reinforcing member 6 is formed into a columnar shape.

さらに通電電流が大きくなると補強部材6の抵抗値も大
きくなり、定格遮断電流Iriになると補強部材6の抵
抗値は約50〔μΩ〕になりコイル電極4の抵抗値より
十分に大きくなる。従って、電流はコイル電極4を流れ
るので電流遮断のために十分な磁界を得ることができる
Furthermore, as the applied current increases, the resistance value of the reinforcing member 6 also increases, and when the rated breaking current Iri is reached, the resistance value of the reinforcing member 6 becomes approximately 50 [μΩ], which is sufficiently larger than the resistance value of the coil electrode 4. Therefore, since the current flows through the coil electrode 4, a sufficient magnetic field can be obtained to interrupt the current.

なお、定格通電電流IrCと定格遮断電流Iriの中間
領域では電極間に生じる磁界は小さいが、この電流範囲
であれば遮断は可能である。
Although the magnetic field generated between the electrodes is small in the intermediate region between the rated energizing current IrC and the rated breaking current Iri, breaking is possible within this current range.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、遮断時は遮断電流により補強部材が高
抵抗値でコイル電極に電流が流れ、通電時は低抵抗値で
ある補強部材に電流が流れるので、通電時におけるコイ
ル電極の電流路における電力損失を低減できる。
According to the present invention, when the current is turned off, current flows through the reinforcing member with a high resistance value due to the breaking current, and when the current is applied, current flows through the reinforcing member with a low resistance value, so that the current path of the coil electrode when the current is applied. power loss can be reduced.

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

第1図は本発明の真空バルブの断面図、第2図は本発明
における寅施例の■203セラミックの通電電流に対す
る抵抗値の変化を示すグラフである。 2・・・接 点 ・・・コイル電極 6・・・補強部材
FIG. 1 is a cross-sectional view of the vacuum valve of the present invention, and FIG. 2 is a graph showing the change in resistance value of the 203 ceramic according to the present invention with respect to the applied current. 2...Contact...Coil electrode 6...Reinforcement member

Claims (1)

【特許請求の範囲】 真空容器内に接離自在に設けられ通電軸に取付けられた
1対の電極の少なくとも一方の背面に通電軸から接続さ
れるコイル電極を有する真空バルブにおいて、 前記通電軸と電極背面間に前記通電軸に接続され且つ前
記コイル電極に嵌入された正の抵抗温度係数を有する補
強部材を設けたことを特徴とする真空バルブ。
[Scope of Claims] A vacuum valve having a coil electrode connected from the current-carrying shaft to the rear surface of at least one of a pair of electrodes that are detachably provided in a vacuum container and attached to the current-carrying shaft, comprising: A vacuum valve characterized in that a reinforcing member having a positive temperature coefficient of resistance is provided between back surfaces of electrodes, the reinforcing member is connected to the current-carrying shaft and fitted into the coil electrode.
JP4128290A 1990-02-23 1990-02-23 Vacuum valve Pending JPH03246840A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4128290A JPH03246840A (en) 1990-02-23 1990-02-23 Vacuum valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4128290A JPH03246840A (en) 1990-02-23 1990-02-23 Vacuum valve

Publications (1)

Publication Number Publication Date
JPH03246840A true JPH03246840A (en) 1991-11-05

Family

ID=12604093

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4128290A Pending JPH03246840A (en) 1990-02-23 1990-02-23 Vacuum valve

Country Status (1)

Country Link
JP (1) JPH03246840A (en)

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