JPS58128615A - Vacuum breaker - Google Patents

Vacuum breaker

Info

Publication number
JPS58128615A
JPS58128615A JP991682A JP991682A JPS58128615A JP S58128615 A JPS58128615 A JP S58128615A JP 991682 A JP991682 A JP 991682A JP 991682 A JP991682 A JP 991682A JP S58128615 A JPS58128615 A JP S58128615A
Authority
JP
Japan
Prior art keywords
electrode
magnetic field
intermediate lead
cylindrical portion
cylindrical
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
JP991682A
Other languages
Japanese (ja)
Inventor
佐野 孝光
横山 寿輝
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 JP991682A priority Critical patent/JPS58128615A/en
Publication of JPS58128615A publication Critical patent/JPS58128615A/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に係り、特にアークに対し平行な
軸方向磁界を発生させる手段を電極の背部に備えてなる
真空しゃ断器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum breaker, and more particularly to a vacuum breaker comprising means for generating an axial magnetic field parallel to an arc at the back of an electrode.

近年、アークにこれと平行な軸方向磁界を印加すること
Kより、アークを電極面上に分散せしめてその局部的な
集中を防止し、もって電極の過度のS−を防ぐことによ
秒しゃ断能力の向上を図った、いわゆるアーク分散方式
(縦磁界方式)の真空しゃ断器が知られている。
In recent years, by applying an axial magnetic field parallel to the arc, it is possible to disperse the arc on the electrode surface and prevent its local concentration, thereby preventing excessive S- on the electrode. A so-called arc dispersion type (vertical magnetic field type) vacuum breaker with improved performance is known.

かかる縦磁界方式の真空しゃ断器は、真空容器内にその
軸線上において1対の電極を接触離反(接離)すべく操
作装置を介し駆動される対をなす電極棒を相対的に接近
離反自在に導入するとともに、各電極とそれぞれの電極
棒の内端部とを、電極棒に流れる軸方向の電流を電極棒
を中心とするループ電流に変更して軸方向磁界を発生さ
せる磁界発生体(コイル体)によ抄接続して構成される
のであるが、従来の縦磁界方式の真空しゃ断器における
コイル体等は、第1図、第2図に示すように設けられて
いた。すなわち、第1図において1は1方の電極棒で、
操作装置を介し他方の電極棒(ともに図示省略)に対し
相対的に接近離反自在に設けられるものであり、その内
端部には、第2図に示すように、円板状の取付部2aと
、この取付部2aの外周の等配した部分から半径方向(
第1図において左右方向)外方へ嬌・伸した複数(第2
図において4本)の腕s2bと、各腕部2bの端部から
相隣る腕部2′bの端部方向へ同一の方向性を有して円
弧状に彎曲した磁界発生部2Cとからなるコイル体2が
、取付11s2aの両面に凹設した凹s3,4の一方を
介して低層されている。また、電極411の内端部には
、大電流を投入、しゃ断すべく真空容器(図示省略)内
において接離される一方の電極5が、その背部(第1図
において下面)中央部に凹設した凹部6とコイル体2に
おける取付部2aの他方の凹部4とに両端を嵌着した1
1m頭円錐体状の雷、極線縁支持体7を介し直列的に固
着されている。そして、コイル体2と電極5とは、コイ
ル体2における各磁界発生部2Cの肩部の孔IK一端を
嵌着するとともに他端を電極5の背部周辺に接合した軸
方向(第1図において上下方向)の通電ビン9を介し接
続されてし)るものである。
In such a vertical magnetic field type vacuum breaker, a pair of electrode rods are driven via an operating device to bring the pair of electrodes into contact with and away from each other on the axis of the vacuum container so that they can be moved relatively toward and away from each other. At the same time, each electrode and the inner end of each electrode rod are connected to a magnetic field generator (which generates an axial magnetic field by changing the axial current flowing through the electrode rod into a loop current centered around the electrode rod). The coil body and the like in a conventional vertical magnetic field type vacuum breaker were provided as shown in FIGS. 1 and 2. That is, in FIG. 1, 1 is one electrode rod,
It is provided so that it can move toward and away from the other electrode rod (both not shown) via an operating device, and has a disk-shaped attachment portion 2a at its inner end, as shown in FIG. radially (
(left and right direction in Figure 1)
From the arms s2b (four in the figure) and the magnetic field generating section 2C curved in an arc shape with the same directionality from the end of each arm 2b toward the end of the adjacent arm 2'b. The coil body 2 is lowered through one of the recesses s3 and 4 recessed on both sides of the mounting 11s2a. Further, at the inner end of the electrode 411, one electrode 5, which is connected and separated in a vacuum container (not shown) in order to input and cut off a large current, is recessed in the center of its back (lower surface in FIG. 1). 1 with both ends fitted into the recess 6 of the coil body 2 and the other recess 4 of the mounting portion 2a of the coil body 2.
1 m cone-shaped lightning bolts are fixed in series via a polar edge support 7. The coil body 2 and the electrode 5 are connected in the axial direction (as shown in FIG. It is connected via the energizing bottle 9 in the vertical direction).

なお、電極絶縁支持体1は、電極5と電極棒1とが電気
的に直接に接続されるのを防止するもので、ステンレス
鋼の如き高抵抗の金属または絶縁物からなるものである
The electrode insulating support 1 prevents the electrode 5 and the electrode rod 1 from being electrically connected directly, and is made of a high-resistance metal such as stainless steel or an insulator.

ところが、上述したコイル体2等を有する真空しゃ断器
においては、コイル体jの磁界発生部za婢の分割数を
多くすると、分割数に反比例して発生する軸方磁界が弱
くなや、シゃ断能力の極端な低下を招来する問題がある
一方、分割数を少なくすると、各磁界発生部20当9の
電流物産が増加し、特に通電ビン9の通電時における通
電容量が不足してその使用に耐え得ない′という問題か
める。
However, in a vacuum breaker having the above-mentioned coil body 2, etc., when the number of divisions of the magnetic field generating part za of the coil body j is increased, the axial magnetic field generated in inverse proportion to the number of divisions becomes weaker, and the axial magnetic field becomes weaker. On the other hand, if the number of divisions is reduced, the current output of each magnetic field generating section 20 and 9 will increase, and the current carrying capacity will be insufficient especially when the energizing bottle 9 is energized, making its use difficult. This raises the issue of not being able to withstand it.

本発明は、上述した間聰に−みてなされたもので、その
目的とするところは、大容量:の電流を優ねたしゃ断性
能でしゃ断し得かつ通電し得るようにした縦磁界方式の
真空しゃ断器を提供するにある。以下、第8図以降の図
面を参照してこの発明の実施例を1#細に説明する。
The present invention has been made in view of the above-mentioned problems, and its object is to provide a vertical magnetic field type vacuum that can cut off large-capacity currents with excellent cutting performance and conduct electricity. Provide a circuit breaker. Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings from FIG. 8 onwards.

本発明に係す真空しゃ断器10は、第3図に示すように
1円柱状の真空容器ll内にその軸線上に位置せしめて
1対の電極棒Uを相対的に接近離反自在に導入し、各電
極棒Uの内端部に大電流を投入。
As shown in FIG. 3, a vacuum breaker 10 according to the present invention has a pair of electrode rods U positioned on the axis of a cylindrical vacuum container 11 so as to be able to approach and separate from each other. , a large current is applied to the inner end of each electrode rod U.

しゃ断すべく接離される対をなす電極13を絶縁物を介
在せしめて直列的に固着するととも罠、各電極棒Uとそ
れぞれの電極13とをwe神tz Kfllれる軸方向
の通電電流を電極棒Uを中心とするループ電流に変更し
て軸方向(箒3図において上下方向)磁界を発生させる
べく各電極肋の背部に配設したコイル体14により接続
して概略構成されている。
When a pair of electrodes 13 that are brought into contact and separated in order to be cut off are fixed in series with an insulator interposed between them, each electrode rod U and each electrode 13 are connected to each other to prevent the axial current flowing through the electrode rods. It is generally constructed by connecting a coil body 14 disposed on the back of each electrode rib in order to generate a magnetic field in the axial direction (in the vertical direction in Figure 3 of the broom) by changing the current to a loop centered on U.

すなわち、真空容器11は、円筒状に成形したガラスま
たはアルミナ質のセラ建ツクスからなる複数(本実施例
においては2個)の絶縁筒IBを、それぞれの両端に植
設したコバールの如き金属材料からなる薄肉円筒状の封
着金具16 、1g 、・・の一方を介して1本の絶縁
筒とするととも罠、その勇−口端を他方の封着金具16
 、16を介し円板状の金属端板17 、17により気
密に封止し、かつ内部を高真空に排気して形成されてい
る。そして、真空容器11内にii、前記対をなす電極
棒Uが各金wI4熾板17の中央に設けた孔17 aか
ら真空容器11の気・特性を保持して相対的に接近離反
自在に導入されている。
That is, the vacuum vessel 11 is made of a metal material such as Kovar, in which a plurality (in this embodiment, two) of insulating cylinders IB made of glass or alumina ceramics formed into a cylindrical shape are implanted at both ends of each insulating cylinder IB. One of the thin cylindrical sealing fittings 16, 1g, . . .
, 16, and are hermetically sealed with disk-shaped metal end plates 17, 17, and the inside is evacuated to a high vacuum. Then, inside the vacuum vessel 11, the pair of electrode rods U can approach and separate from each other through a hole 17a provided in the center of each gold wI4 plate 17 while maintaining the gas characteristics of the vacuum vessel 11. It has been introduced.

なお、一方(第3図において上方)の電極棒Uは、一方
の金11端板17に気密に接合されているものであり、
他方の直極伸Uは、音域ベローズ18により真?!谷器
1】の気密性を保持しつつ他方の音域端板17の孔17
 aを軸方向へ移動自在に挿通されるとともに、真空容
器11の外部に配設される図示しない操作装置を介し往
復駆動されるものである。
Note that one electrode rod U (upper in FIG. 3) is hermetically joined to one gold 11 end plate 17,
Is the other straight pole extension U true due to the range bellows 18? ! hole 17 of the other sound range end plate 17 while maintaining the airtightness of the valley device 1]
It is inserted through the tube so as to be freely movable in the axial direction, and is driven back and forth via an operating device (not shown) disposed outside the vacuum container 11.

また、第3図において川は電極u、13等を同心状に囲
繞する円筒状の主シールドで、その中間部付近を@記一
方の封着金具16に挾持されたリング円板状の支持金真
夏により支持されるものであり、21 、21 ij各
金輿端板17の内面に固着した補助シールドである。
In addition, in FIG. 3, the main shield is a cylindrical main shield that concentrically surrounds the electrodes u, 13, etc., and the ring disk-shaped support metal sandwiched between the sealing metal fittings 16 on one side is located near the middle part of the main shield. It is supported by Midatsu, and is an auxiliary shield fixed to the inner surface of each metal palanquin end plate 17.

峠配他方(可動側)の電極棒12の内端部には、第4図
に示すように、 1lTeコイル体14の一部を構成す
る有底円筒状の中間リード体nが1斤部−1!2 a 
(7)外面(第4図において下面)中央に凹設した凹部
23を介し嵌合されかつろう付けによね固着されており
、この中間リード体nは、オーステナイト系ステンレス
鋼の如く機械的強度大にしてかつ高抵抗の金輌からなる
とともに電極棒12の内端部付近に嵌着したリング円板
状の補強金具24 Kよりその底部外面をろう付は接合
されて補強支持されている。中間リード体nの底部1r
2ILの内面中央には、その外面と同様に四部5を凹設
してあ沙、この凹部5には、@紀電極13を電極棒12
に対して電気的に絶縁して直列的に支持すべく、両端に
7ランジ部35aを一体成形したオーステナイト系ステ
ンレス鋼の如く高抵抗の金属または絶縁物からなる円筒
状の電極絶縁支持体Xが、一端の7ランジ部為を介し嵌
合されかつろう付けにより固着されている。電極絶縁支
持体Xの他喝の7ランジ[)には、電極■が、その背部
中央付近に中間リード体nの筒@6xbより小径に一体
成形した筒部13 aを介し嵌合されかつろう付けによ
り固着されており、劃13の筒部13 aは、中間リー
ド体nの筒部gbと半径方向(第4図において左右方向
)において同心状に重畳せしめられている。そして、電
極13ふ の筒部13と中間リード体nの筒部22bとは、中間リ
ード体1と相俟って前記コイル体14を構成する磁界発
生体WKよ抄電気的に接続されている。磁界発生体1は
1通電電流の経路を変更して軸方向磁界を発生させるも
ので、第4図、第5図に示すように、中間リード体ff
Kおける筒部x’bの段部Xを設けた内周面および11
1極13における筒部13 mの外周面Kl装してろう
付けにより固着される外リング部1aおよび内リング部
7!7bと、各りング部W a 、 2I b間を接続
すべく周方向へ同一の方向性を保持しかつ等配して設け
たスパイラル状の複数1本実施例においては2個)の磁
界発生部IOとからな抄、プレス成形等により導電板か
ら一体成形した複数(本実施例においては2個)の磁界
発生素体を軸方向へ重畳して設けられている。
As shown in FIG. 4, at the inner end of the electrode rod 12 on the other side (movable side) of the pass, there is a 1 loaf portion of a bottomed cylindrical intermediate lead body n that constitutes a part of the 11Te coil body 14. 1!2 a
(7) It is fitted through a recess 23 formed in the center of the outer surface (lower surface in FIG. 4) and is firmly fixed by brazing, and this intermediate lead body n is made of high mechanical strength such as austenitic stainless steel. The bottom outer surface of the electrode rod 12 is brazed and reinforced by a ring-disc-shaped reinforcing metal fitting 24K which is made of high-resistance metal and fitted near the inner end of the electrode rod 12. Bottom part 1r of intermediate lead body n
In the center of the inner surface of the 2IL, a four part 5 is recessed in the same way as the outer surface.
A cylindrical electrode insulating support X made of a high-resistance metal or insulator such as austenitic stainless steel is integrally formed with seven flange portions 35a at both ends in order to electrically insulate and support the electrode in series. , are fitted through seven flange portions at one end and fixed by brazing. The electrode (2) is fitted into the 7th flange [) of the electrode insulating support X through a cylindrical portion 13a which is integrally formed near the center of its back and has a smaller diameter than the cylinder @6xb of the intermediate lead body n. The cylindrical portion 13a of the stem 13 is concentrically overlapped with the cylindrical portion gb of the intermediate lead body n in the radial direction (left-right direction in FIG. 4). The cylindrical portion 13 of the electrode 13 and the cylindrical portion 22b of the intermediate lead body n are electrically connected to the magnetic field generator WK, which together with the intermediate lead body 1 constitutes the coil body 14. . The magnetic field generator 1 generates an axial magnetic field by changing the path of the current flowing through it, and as shown in FIGS. 4 and 5, the intermediate lead body ff
The inner circumferential surface of the cylindrical portion x'b in K with the stepped portion X and 11
In order to connect the outer ring part 1a and the inner ring part 7!7b which are mounted on the outer peripheral surface Kl of the cylindrical part 13m in one pole 13 and fixed by brazing, and each ring part W a, 2I b, the circumferential direction is A plurality of spiral-shaped magnetic field generating parts IO (two in this embodiment) are arranged uniformly and with the same directionality, and a plurality of spiral-shaped magnetic field generating parts IO (two in this embodiment) are integrally formed from a conductive plate by karana-shaping, press molding, etc. In this embodiment, two (2) magnetic field generating element bodies are provided so as to be superimposed in the axial direction.

なお、第4図、第5図においてΔは電極絶縁支持体Xの
中間リード体n等とのろう付は時のガス抜き孔、Xは磁
界発生体2yVCおける内りング部W。
In FIGS. 4 and 5, Δ is a gas vent hole when the electrode insulating support X is brazed to the intermediate lead n, etc., and X is the inner ring W in the magnetic field generator 2yVC.

の内周縁に開成した切欠きで、電極13の筒部13 a
との接合時にろう材を収納するためのものである。
The cylindrical portion 13 a of the electrode 13 is formed with a notch formed on the inner peripheral edge of the
This is to store the brazing filler metal during bonding.

また、一方(固定側)の電極棒12の内端部に固着され
る電極13およびコイル体14等は、上述した他方のも
のとほぼIWJ様であるのでその説明を省略する◎ 以上の構成からなる真空しゃ断器10は、従前の真空し
ゃ断器と同様に対をなす′li1& 13を操作装置に
よね圧接して大容量の電流を通電し、また他方の電極1
3を一方の電&13から操作装置により瞬時に離反せし
めて大容量の電流をしゃ断するものであるが、通電時に
電極@ 12と電極13を接続するコイル体14の磁界
発生体14がその通路断面積を大きく設けてあり、かつ
筒部13 a 、 22 ’bを介して電極柳菫2等と
接続しであるので、発熱等によりその使用に耐え得ない
ということはない。また、磁界発生体1の磁界発生部N
oによ抄発生する軸方向磁界は、全電流が2個の磁界発
生部27 c K分流するものであるから、その強度が
低下するおそれはなく、シゃ断能力も良好となるもので
ある。
In addition, the electrode 13 and coil body 14 fixed to the inner end of one (fixed side) electrode rod 12 are similar to the other one described above, so their explanation will be omitted.◎ From the above configuration The vacuum breaker 10 has a pair of electrodes 1 and 13 pressed against an operating device to supply a large amount of current in the same manner as the previous vacuum breaker.
3 is instantaneously separated from one of the electrodes &13 by an operating device to cut off a large amount of current. However, when electricity is applied, the magnetic field generator 14 of the coil body 14 that connects electrode @12 and electrode 13 breaks the path. Since it has a large area and is connected to the electrode violet 2 etc. via the cylindrical portions 13a and 22'b, it will not become unusable due to heat generation or the like. In addition, the magnetic field generating portion N of the magnetic field generating body 1
Since the total current of the axial magnetic field generated by o is divided into two magnetic field generating parts 27c, there is no risk of its strength decreasing, and the cutting ability is also good. .

なお、前述した実施例においては、電極13の筒部13
 aの外径をコイル体14における中間リード体〃の筒
部22bの内径より小径に形成して設けた場合について
述べたが、これに限定されるものではなくたとえば電極
13の筒部13 aの内径を中間リード体四の筒部22
bの外径より大径に形成して設けるとともに、両者間に
磁界発生体Iを介装してもよいものである。また、磁界
発生体Iは、磁界発生素体を1個としてもよいとともに
、その外リング部、27aと内リング部1bとを接続す
る磁界発生部7?7Cを2個とする場合に限らず1個ま
たは311以上としてもよいものである。さらに、磁界
発生体lは、その磁界発生部ffcをスパイクに状に形
成する場合に限らずたとえば第6図に示すように、外リ
ング部27−と内りング部h′とを両4に#−径方向の
接続部を備えた1個の有熾環状の磁界発生gl+ 27
 c ’により接続した磁界発生体l′としてもよいも
のである。また、磁界発生体;v、27′は、外リング
部27 a 、 ffa’、内リング部;vb、zyb
’および磁界発生部27 c 、 ffc’を一体成形
する場合に限らず、別個に成形した各部を接合して一体
的に設けてもよいものであるとともに、磁界発生部27
 a 、 ffc’のみによし磁界発生体としてもよい
ものである。
In addition, in the embodiment described above, the cylindrical portion 13 of the electrode 13
Although the case where the outer diameter of a is smaller than the inner diameter of the cylindrical portion 22b of the intermediate lead body in the coil body 14 has been described, the present invention is not limited to this. The inner diameter is the cylindrical part 22 of the intermediate lead body 4.
It may be formed to have a larger diameter than the outer diameter of b, and the magnetic field generator I may be interposed between the two. Further, the magnetic field generating body I may have one magnetic field generating element, and is not limited to two magnetic field generating units 7 to 7C connecting the outer ring portion 27a and the inner ring portion 1b. The number may be 1 or 311 or more. Furthermore, the magnetic field generating body l is not limited to the case where the magnetic field generating portion ffc is formed in the shape of a spike. For example, as shown in FIG. # - 1 annular magnetic field generator gl+ with radial connection 27
It may also be used as a magnetic field generator l' connected by c'. Further, magnetic field generators; v, 27' are outer ring parts 27a, ffa', inner ring parts; vb, zyb
' and the magnetic field generating parts 27c, ffc' are not limited to being integrally molded, and may be provided integrally by joining each part molded separately, and the magnetic field generating part 27
It is also possible to use only a and ffc' as a magnetic field generator.

第7図は本発明の第2実施例の壁部縦断面図で、この実
施例のものは、コイル体14における磁界発生体i、v
’を軸方向へ離隔して設けた2個とするとともに、両者
間をリング円板状の接続導体πにより直列接続すること
Kよって、軸方向磁界の強賓を向上せしめたこと等が前
述した第1実施例のものと相違するものであるから、第
1実施例のものと同一の機能を!する部材には同一符号
を付してその説明を省略する。
FIG. 7 is a longitudinal cross-sectional view of a wall of a second embodiment of the present invention, in which the magnetic field generators i and v in the coil body 14 are
As mentioned above, the strength of the axial magnetic field was improved by making two pieces separated in the axial direction and connecting them in series with a ring-disc-shaped connection conductor π. Since it is different from the first embodiment, it has the same function as the first embodiment! The same reference numerals are used to denote the same members, and the explanation thereof will be omitted.

すなわち、径を違えて設けた電極13の筒部13mの端
部とコイル体14における中間リード体nの筒部22b
の端部とは、軸方向へ離隔して設けられており、それぞ
れの筒部13a、Mbには、磁界発生体y 、、t+y
’が内リング部zyb、:vb’または外リング部27
a 、 j!7a ’を介して嵌着されている。そして
、電極13の筒部13 aに嵌着した磁界発生体1,1
′の外リング部27 a 、 ffa’と中間リード体
nの筒部zbK嵌着した磁界発生体y 、y’の内リン
グ部yb。
That is, the ends of the cylindrical portion 13m of the electrode 13 provided with different diameters and the cylindrical portion 22b of the intermediate lead body n in the coil body 14.
are provided spaced apart from the end portions in the axial direction, and the respective cylindrical portions 13a, Mb include magnetic field generators y, , t+y
' is the inner ring part zyb, :vb' or the outer ring part 27
a, j! It is fitted through 7a'. Then, the magnetic field generators 1, 1 fitted into the cylindrical portion 13a of the electrode 13
The outer ring portions 27a and ffa' of the magnetic field generating body y and the inner ring portion yb of y' are fitted into the cylindrical portion zbK of the intermediate lead body n.

yb’とは、前記りング円板状の接続導体犯における外
周縁および内周縁に互いに異なる軸方向へ襲用して形成
した突縁31 a 、 31 bを介し電気的に接続さ
れている。
yb' is electrically connected to the ring disk-shaped connecting conductor via projecting edges 31 a and 31 b formed on the outer and inner edges of the connecting conductor in different axial directions.

なお、上述した第2実施例においては、電極13のrW
J部13 aの外径を中間リード体2の筒部22bの内
径より小径に形成して設けた場合を例示したが、こねに
限らず電極18の筒部13 aの内径を中間リード体n
の筒部2bの外径より大径に形成して設けてもよいもの
である。また、磁界発生体y 、 27’は、前述した
fIIJ1実施例のものと同様に設けてよいものである
が、外リング部ffaおよび内リング部ybtよ、少な
くともいずれか一方を設ければよいものである。
Note that in the second embodiment described above, the rW of the electrode 13
Although the case where the outer diameter of the J part 13a is formed to be smaller than the inner diameter of the cylindrical part 22b of the intermediate lead body 2 is illustrated, the inner diameter of the cylindrical part 13a of the electrode 18 is not limited to kneading.
It may be formed to have a larger diameter than the outer diameter of the cylindrical portion 2b. Further, the magnetic field generators y and 27' may be provided in the same manner as those in the fIIJ1 embodiment described above, but it is sufficient to provide at least one of the outer ring part ffa and the inner ring part ybt. It is.

以上の如く本発明は、真空容器内に1対の電極棒を軸線
上に位置せしめて相対的に接近離反自在底 に導入し、前記各電極棒の内端部に、有熾円筒状の中間
リード体をそれぞれの開口端を対向せしめてX心的に固
着するとともに、各中間リード体の筒部と径を違えたf
llIIlを背部に備えた11極をそれぞれの筒部を各
中間リード体の筒部と半径方向において同心状に重畳せ
しめて電極絶縁支持体を介し直列的に固着し、前記各中
間リード体の筒部とそれぞれの111に!の筒部との間
を1個または複数個のスパイラル状もしくは1個の有端
環状の磁界発生体により接続して設けたものであるから
、通電電流の容量を抵抗熱等の発生を伴なうことなく容
易に増大せしめることができ、ひいてri縦磁界方式の
真空しゃ断器を通電容量およびしゃ断能力に優れたもの
へすることができる。
As described above, in the present invention, a pair of electrode rods are positioned on the axis in a vacuum container and introduced into the bottom which can be moved toward and away from each other, and a rounded cylindrical intermediate portion is attached to the inner end of each electrode rod. The lead bodies are fixed in an X-centered manner with their open ends facing each other, and the cylindrical part and diameter of each intermediate lead body are different from each other.
11 poles each having 11 poles on the back are fixed in series through an electrode insulating support with their respective cylindrical parts superimposed concentrically in the radial direction with the cylindrical parts of each intermediate lead body, and the cylindrical parts of each intermediate lead body are Department and each 111! Since the cylindrical part is connected to the cylindrical part by one or more spiral or one end ring-shaped magnetic field generating body, the capacity of the current flowing can be controlled without causing resistance heat etc. Therefore, the RI vertical magnetic field type vacuum breaker can be made to have excellent current carrying capacity and breaking ability.

また、真空容器内に1対の電極棒を軸線上に位置せしめ
て相対的に接近離反自在に導入し、前記各電極棒の内端
部に、有底円筒状の中間リード体をそれぞれの開口端を
対向せしめて同心的に固着するとともに、各中間リード
体の筒部と径を違えた筒部を背部に備えた電極をそれぞ
れの筒部の1部を各中間リード体の筒部の1部と軸方向
へ離隔せしめて電極絶縁支持体を介し直列的に固着し、
前記各中間リード体の筒部およびそれぞれの電極のm1
@w外リングおよび内リングの双方またはいずれか一方
を備えた1個または複数個のスノ(イラル状もしくは1
個の有備環状の磁界発生体を嵌着し、前記各中間リード
体の筒部に嵌着した磁界発生体とそれぞれの電極の筒部
に嵌着した磁界発生体とをリング円板状にしてかつ内W
8縁および外周縁に9嫌を備えた接続導体により直列接
続して設けたものであるから、上述した効JllK加え
て軸方向磁界の強蜜を大幅に向上することができる婢の
効果を奏する。
Further, a pair of electrode rods are positioned on the axis line and introduced into the vacuum container so as to be able to approach and separate from each other, and a bottomed cylindrical intermediate lead body is attached to the inner end of each electrode rod at each opening. The electrodes are fixed concentrically with their ends facing each other, and have a cylindrical part on the back having a diameter different from that of the cylindrical part of each intermediate lead body. The electrodes are separated from each other in the axial direction and fixed in series through an electrode insulating support.
m1 of the cylindrical portion of each intermediate lead body and each electrode
@w One or more snowsocks (iral shaped or single) with outer ring and/or inner ring.
The magnetic field generators fitted in the cylindrical portion of each intermediate lead body and the magnetic field generators fitted in the cylindrical portions of the respective electrodes are formed into a ring disk shape. Inside W
Since they are connected in series by connecting conductors with 8 edges and 9 holes on the outer periphery, in addition to the above-mentioned effect, the strength of the axial magnetic field can be greatly improved. .

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

第1図は従来の真空しゃ断器の装部縦断面図で、第2図
はその1−1線矢視図、第3図は本発明に係る真空しゃ
断器の縦断面図、@4図および縞5図は本発明の第1実
施例における要部の縦断面図および平面図、第6図は第
1実施例における壁部の他の実施例の平面図、第7図は
本発明の第2実施例におけるlLF部のIIX断面図で
ある01]・・・真空容器、!2・・・電極棒、13・
・・電極、131・・筒部、n・・・中間リード体、M
b・・・筒部、X・・・電極絶縁支持体、W、W’・・
・磁界発生体、 ff a 、 J7a’・・・外りン
グ部、y b 、 yb’・・・内リング部、2’i 
o 、 2fa’・・・磁界発生部、J・・・接続導体
、31 a 、 31 b、・・・突縁。 第3図
Fig. 1 is a longitudinal cross-sectional view of the conventional vacuum breaker, Fig. 2 is a view taken along the line 1-1, and Fig. 3 is a longitudinal cross-sectional view of the vacuum breaker according to the present invention. Stripe 5 is a vertical cross-sectional view and a plan view of the main part in the first embodiment of the present invention, FIG. 6 is a plan view of another embodiment of the wall portion in the first embodiment, and FIG. 01 which is an IIX cross-sectional view of the lLF section in Example 2]...Vacuum vessel,! 2... Electrode rod, 13.
...Electrode, 131...Cylinder part, n...Intermediate lead body, M
b...Cylinder part, X...Electrode insulating support, W, W'...
・Magnetic field generator, ffa, J7a'...outer ring part, yb, yb'...inner ring part, 2'i
o, 2fa'...Magnetic field generation part, J...Connection conductor, 31a, 31b,...Protrusion. Figure 3

Claims (1)

【特許請求の範囲】 (1)真空容器内に1対の電極棒を軸線上に位置せしめ
て相対的に接近離反自在に導入し、前記底 各電極棒の内端部に、有端円筒状の中間リード体をそれ
ぞれの開口端を対向せしめて同心的に固着するとともに
、各中間リード体の筒部と径を違えた筒部を背部に備え
た電極をそれぞれの筒部を各中間リード体の筒部と半径
方向において同心状に重畳せしめて電極絶縁支持体を介
し直列的に固着し、前記各中間リード体の筒部とそれぞ
れの電極の筒部との間を1個才たけ複数個のスパイラル
状もしくけ1個の有端環状の磁界発生体に上り接続して
設けたことを特徴とする真空しゃ断器。 (2)各中間リード体の筒部の内径をそれぞれの電極の
筒部の外径より大梗に形成したことを特徴とする特許請
求の範囲第1項記載の真空しゃ断器。 (3)各中間リード体の筒部の外径をそれぞれの電極の
筒部の内径より小径に形成したことを特徴とする特許請
求の範囲第1項記載の真空しゃ断器。 (4)各磁界発生体を軸方向へ重畳した複数個のスト 磁界発生稟子により形成したことを特徴とする特許請求
の範囲第1項から第3項までのいすわかに記載の真空し
ゃ断器。 (5)各磁界発生体をそれぞれの中間リード体の筒部ま
たは電極の筒部に嵌着される外リング部および内リング
部を備えたものとしたことを特徴とする特許請求の範囲
第1項から第4項までのいずれかに記載の真空しゃ断器
。 (611I?容器内に1対のt極柳を軸線上に位置せし
めて相対的に接近離反自在に導入し、I!II記各電極
柳の内端部に、有底円筒状の中間リード体をそれぞれの
開口喝を対向せしめて同心的に固着するとともに、各中
間リード体の筒部と径を違えた筒部を背部に備えた電極
をそれぞれの筒部の端部を各中間リード体の筒部の端部
と軸方向へ#1llil!せしめて電極絶縁支持体を介
し直列的に固着し、#記各中間リード体の筒部および護
り それぞれの電極の筒部に外リングおよび内りン、、!ヱ グの双方またはいずれか一方を備えた1個または複数個
のスパイラル状もしくは1個の有端環状の磁界発生体を
嵌着し、前記各中間リード体の筒部に嵌着した磁界発生
体とそれぞれの電極の筒部に嵌着した磁界発生体とをリ
ング円板状にしてかつ内局縁および外周縁に突縁を備え
た接続導体により直列接続して設けたことを特徴とする
真空しゃ断器。 (7)各中間リード体の筒部の内径をそれぞれの電極の
筒部の外径より大径に形成したことを特徴とする特許請
求の範囲第6項記載の真空しゃ断器。 (8)各中間リード体の筒部の外径をそれぞれの電極の
筒部の内径より小径に形成したことを特徴とする特許請
求の範囲第6項記載の真空しゃ断器。 (9)各磁界発生体を軸方向へ重畳した複数個の磁界発
生素体により形成したことを特徴とする特許請求の範囲
第6積から第8項までのいずれかに記載の真空しゃ断器
[Scope of Claims] (1) A pair of electrode rods are positioned on the axis line and introduced into a vacuum container so as to be able to approach and separate from each other, and a cylindrical shape with an end is inserted into the inner end of each electrode rod at the bottom The intermediate lead bodies are fixed concentrically with their open ends facing each other, and electrodes each having a cylindrical part on the back having a diameter different from that of the cylindrical part of each intermediate lead body are attached to each intermediate lead body. The cylindrical portion of each intermediate lead body and the cylindrical portion of each electrode are overlapped concentrically in the radial direction and fixed in series through an electrode insulating support. 1. A vacuum breaker, characterized in that the spiral structure is connected upwardly to one end-shaped annular magnetic field generator. (2) The vacuum breaker according to claim 1, wherein the inner diameter of the cylindrical portion of each intermediate lead body is larger than the outer diameter of the cylindrical portion of each electrode. (3) The vacuum breaker according to claim 1, wherein the outer diameter of the cylindrical portion of each intermediate lead body is formed to be smaller than the inner diameter of the cylindrical portion of each electrode. (4) The vacuum breaker according to Claims 1 to 3, wherein each magnetic field generating body is formed by a plurality of magnetic field generating rods superimposed in the axial direction. (5) Each magnetic field generating body is provided with an outer ring part and an inner ring part that are fitted into the cylinder part of the respective intermediate lead body or the cylinder part of the electrode. The vacuum breaker according to any one of Items 1 to 4. (611 I? A pair of electrode willows are positioned on the axis line and introduced into the container so that they can approach and separate from each other freely, and a bottomed cylindrical intermediate lead body is attached to the inner end of each electrode willow in I! are fixed concentrically with their openings facing each other, and an electrode with a cylindrical part on the back having a diameter different from that of the cylindrical part of each intermediate lead body is connected to the end of each cylindrical part of each intermediate lead body. #1llil! is fixed in series with the end of the cylindrical part in the axial direction via the electrode insulating support, and the outer ring and inner ring are attached to the cylindrical part of each intermediate lead body marked with # and the cylindrical part of each electrode. ,,! One or more spiral-shaped or one end-ring-shaped magnetic field generating body equipped with both or either one of the above-mentioned intermediate lead bodies is fitted into the cylindrical portion of each of the intermediate lead bodies. The magnetic field generating body and the magnetic field generating body fitted into the cylindrical portion of each electrode are formed into a ring disk shape and are connected in series by a connecting conductor having a protruding edge on the inner center edge and the outer circumferential edge. (7) The vacuum breaker according to claim 6, characterized in that the inner diameter of the cylindrical portion of each intermediate lead body is formed to be larger than the outer diameter of the cylindrical portion of each electrode. (8) The vacuum breaker according to claim 6, characterized in that the outer diameter of the cylindrical portion of each intermediate lead body is formed to be smaller than the inner diameter of the cylindrical portion of each electrode. (9) The vacuum breaker according to any one of claims 6 to 8, wherein each magnetic field generating body is formed by a plurality of magnetic field generating elements superimposed in the axial direction.
JP991682A 1982-01-25 1982-01-25 Vacuum breaker Pending JPS58128615A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP991682A JPS58128615A (en) 1982-01-25 1982-01-25 Vacuum breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP991682A JPS58128615A (en) 1982-01-25 1982-01-25 Vacuum breaker

Publications (1)

Publication Number Publication Date
JPS58128615A true JPS58128615A (en) 1983-08-01

Family

ID=11733415

Family Applications (1)

Application Number Title Priority Date Filing Date
JP991682A Pending JPS58128615A (en) 1982-01-25 1982-01-25 Vacuum breaker

Country Status (1)

Country Link
JP (1) JPS58128615A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5296369A (en) * 1976-02-03 1977-08-12 Hazemeijer Bv Vacuum switch
JPS5627629U (en) * 1979-08-08 1981-03-14

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5296369A (en) * 1976-02-03 1977-08-12 Hazemeijer Bv Vacuum switch
JPS5627629U (en) * 1979-08-08 1981-03-14

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