JPS5938688B2 - vacuum circuit breaker - Google Patents

vacuum circuit breaker

Info

Publication number
JPS5938688B2
JPS5938688B2 JP48142569A JP14256973A JPS5938688B2 JP S5938688 B2 JPS5938688 B2 JP S5938688B2 JP 48142569 A JP48142569 A JP 48142569A JP 14256973 A JP14256973 A JP 14256973A JP S5938688 B2 JPS5938688 B2 JP S5938688B2
Authority
JP
Japan
Prior art keywords
contact
arc
shaped
contacts
outer periphery
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
Application number
JP48142569A
Other languages
Japanese (ja)
Other versions
JPS4996271A (en
Inventor
ウエイン クロ−チ ドナルド
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.)
General Electric Co
Original Assignee
General Electric Co
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 General Electric Co filed Critical General Electric Co
Publication of JPS4996271A publication Critical patent/JPS4996271A/ja
Publication of JPS5938688B2 publication Critical patent/JPS5938688B2/en
Expired 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
    • H01H33/6643Contacts; Arc-extinguishing means, e.g. arcing rings having disc-shaped contacts subdivided in petal-like segments, e.g. by helical grooves

Description

【発明の詳細な説明】 発明の背景 この発明は真空遮断器、更ζこ具体的に云えば、遮断の
際に形成されたアークを回転させる溝孔つき円板形接点
で構成される形式の大電流真空遮断器に関する。
BACKGROUND OF THE INVENTION The present invention relates to a vacuum circuit breaker, more specifically of the type consisting of a slotted disc-shaped contact which rotates the arc formed during interruption. Regarding large current vacuum circuit breakers.

全般的にこの形式を持つ接点構造が米国特許第2949
520号に記載されている。
A contact structure generally having this type is disclosed in U.S. Patent No. 2949.
No. 520.

この特許の各接点は円板形部材で構成され、円板形部材
の半径方向並びに円周方向の両方に伸びる複数個の溝孔
が設けられている。
Each contact in this patent is comprised of a disc-shaped member with a plurality of slots extending both radially and circumferentially of the disc-shaped member.

これらの溝孔は、円板形部材の溝孔つき部分に末端を持
つアークを強制的に円板形部材の中心軸線の周りに回転
させるアーク回転効果を発生させる為に使われている。
These slots are used to create an arc rotation effect that forces an arc terminating in the slotted portion of the disc to rotate about the central axis of the disc.

円板形部材の中心にボタン状の環状接触部があり、回路
遮断動作の際にこSでアークが開始される。
At the center of the disk-shaped member is a button-shaped annular contact, at which an arc is initiated during a circuit breaking operation.

このアークがボタン状接触部から半径方向外向きOこ磁
気的に、駆動され、円板形部材の外周に近づくと、円板
形部付内の溝孔によって発生されるアーク回転作用によ
って回転させられる。
This arc is magnetically driven radially outward from the button-shaped contact, and as it approaches the outer circumference of the disc-shaped member, it is rotated by the arc rotation action generated by the slot in the disc-shaped member. It will be done.

前掲米国特許の接点構造を改良した形が米国特許第35
22399号に記載されている。
U.S. Patent No. 35 is an improved version of the contact structure of the aforementioned U.S. patent.
No. 22399.

この特許の接点構造では、各々の円板形接点に4つの溝
孔が設けられる。
In the contact structure of this patent, each disc-shaped contact is provided with four slots.

各々の溝孔は、接点の外周上の出発点から、ボタン状接
触部の外周に対して大体接線方向の通路をたどって接点
の本体内に入り込む形を持っている。
Each slot is configured to enter the body of the contact from a starting point on the outer periphery of the contact, following a path generally tangential to the outer periphery of the button-like contact.

その一番内側の端に、溝孔は溝孔の接線部分の横方向に
、ボタン状接触部の周縁より半径方向内側に隔たる点ま
で伸びる部分を有する。
At its innermost end, the slot has a portion extending transversely of the tangential portion of the slot to a point spaced radially inwardly from the periphery of the button contact.

後に挙げた米国特許の接点構造は、所望のアーク回転作
用を発生させるのに一般的に非常に有効であるが、この
構造がこの点で望まれる程有効でないと思われる特定の
1つの遮断器の用途がある。
Although the contact structure of the U.S. patent listed below is generally very effective in producing the desired arc rotation action, there is one particular circuit breaker in which this structure does not appear to be as effective as desired in this regard. It has several uses.

この用途は、接点を取巻く普通の管状の金属遮蔽体が接
点から短い距離だけ隔たる大電流真空遮断器(即ち非対
称係数が最大1.3であって実効値が160000アン
ペアより大きい遮断電流の定格を持つ遮断器)の場合で
ある。
This application is used in high-current vacuum circuit breakers (i.e., with an asymmetry factor of up to 1.3 and a rated breaking current greater than 160,000 amperes rms) in which an ordinary tubular metal shield surrounding the contacts is separated from the contacts by a short distance. This is the case for circuit breakers with

この用途では、大電流アークが過度に隣接した遮蔽体を
溶かし且つこがす傾向があるように思われる。
In this application, it appears that high current arcs tend to melt and burn excessively adjacent shields.

この著しい傾向の原因として考えられるのが、接点の周
縁上にその領域のアークを半径方向外向きに追いやる磁
力成分がアークを円周方向に追いやる磁力成分に較べて
大きい領域があることであることが、発明者の研究から
判った。
A possible reason for this remarkable tendency is that there is a region on the periphery of the contact where the magnetic force component that drives the arc outward in the radial direction is larger than the magnetic force component that drives the arc circumferentially. This was determined from the inventor's research.

半径方向外向きに作用するこの大きな力成分が、遮蔽体
の内面にアークを吹付け、その場所で遮蔽体の壁の力ロ
熱及び侵食を増加させる。
This large force component, acting radially outward, arcs the inner surface of the shield, increasing the force heating and erosion of the shield wall at that location.

遮蔽体材料の蒸発による圧力が高まると、アークの円周
方向の移動が阻害され、この為遮蔽体の面の内、この局
部的な領域に対する熱入力の割合が高くなる。
The increased pressure due to evaporation of the shield material inhibits circumferential movement of the arc, thereby increasing the rate of heat input to this local area of the shield surface.

この為にアークが更に遅くなり、この局部領域に於ける
遮蔽体の侵食が一層甚だしくなり、その為遮蔽体の局部
領域での加熱効果がピラミッド状に増大する。
This causes the arc to slow down further and the erosion of the shield in this local area to be more severe, so that the heating effect in the local area of the shield increases pyramidally.

発明の概要 この発明の目的は、前掲米国特許第3522399号に
記載される形の溝孔を使っても、並びに接点の外周とそ
れを取巻く管状遮蔽体の間のすき間が小さくても、不当
な失速を伴わずに、大電流アークを接点の周縁に沿って
高速で回転させることが出来る接点装置を提供すること
である。
SUMMARY OF THE INVENTION It is an object of the present invention to avoid undue interference even with the use of slots of the type described in U.S. Pat. To provide a contact device capable of rotating a large current arc along the periphery of a contact at high speed without stalling.

別の目的は、全体としては前掲米国特許第35223’
99号に記載された形であるが、大電流を遮断する際、
遮蔽体に対するアーク・エネルギを遮蔽体の全周にわた
って一層均一に分布させ、こうして遮蔽体の過度の溶融
並びに焼損を避けるような形で接点を用いることである
Another purpose is to provide a solution to the invention, generally referred to in U.S. Pat. No. 35,223'
This is the form described in No. 99, but when interrupting a large current,
The use of contacts is such that the arc energy to the shield is more evenly distributed over the entire circumference of the shield, thus avoiding excessive melting and burnout of the shield.

この発明を1形式で実施する時、大電流真空遮断器が2
つの円板形接点で構成され、その各々が少なくとも6.
35cm(2,5インチ)より大きい直径を持つと共に
、いづれも前掲米国特許第3522399号に記載され
たものと同様な形の4つのアーク回転用溝孔を有する。
When implementing this invention in one form, two large current vacuum circuit breakers are used.
It consists of three disc-shaped contacts, each of which has at least 6.
It has four arc rotation slots having a diameter greater than 35 cm (2.5 inches) and each having a shape similar to that described in U.S. Pat. No. 3,522,399, cited above.

通常は、接点とは電気的に導通してない管状金属遮蔽体
が、接点を小さな空間を介して取囲んでいる。
Typically, a tubular metal shield, which is not in electrical communication with the contacts, surrounds the contacts through a small space.

両接点の周縁は実質的に整合しているが、互いに円周方
向にずらされ、一方の接点の周縁上に於ける溝孔の出発
点が他方の接点の周縁上に於ける溝孔の出発点から35
°乃至55°ずれるようにする。
The circumferential edges of both contacts are substantially aligned but circumferentially offset from each other such that the starting point of the slot on the circumferential edge of one contact is the same as the starting point of the slot on the circumferential edge of the other contact. 35 from the point
The angle should be between 55° and 55°.

実施例の記載 この発明を一層よく理解されるように、次に図面につい
てこの発明を説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS In order that the invention may be better understood, it will now be described with reference to the drawings.

第1図に、10−’トル又はそれ以下の圧力にまで真空
にされた密封外被10を持つ真空遮断器が示されている
In FIG. 1, a vacuum circuit breaker is shown having a sealed envelope 10 evacuated to pressures of 10-' Torr or less.

この外被10は絶縁材料の管状ケーシング11と、ケー
シング11の両端に適当な耐真空封じ14によって結合
された1対の端蓋12及び13とで構成される。
The jacket 10 consists of a tubular casing 11 of insulating material and a pair of end caps 12 and 13 connected to opposite ends of the casing 11 by suitable vacuum seals 14.

外被10の中に相対的に可動の1対の接点17及び1B
が設けられる。
A pair of relatively movable contacts 17 and 1B within the jacket 10
is provided.

これらの接点が第1図では離脱状態又は開路状態を実線
で示しである。
These contacts are shown in solid lines in FIG. 1 when in a disconnected or open state.

上側接点17が導電棒17aに適当に取付けられた固定
接点であり、導電棒17aの上端が上側端蓋12に結合
される。
The upper contact 17 is a fixed contact suitably attached to a conductive rod 17a, and the upper end of the conductive rod 17a is coupled to the upper end cap 12.

下側接点18が導電性の作動棒18aに取付けられた可
動接点であり、この作動棒18aが垂直方向に移動出来
るように適当に取付けられている。
The lower contact 18 is a movable contact mounted on a conductive actuation rod 18a, which is suitably mounted for vertical movement.

接点18が実線で示す位置から破線で示す位置へ上向き
に移動すると、接点が係合し、こうして遮断器が閉じる
が、下向きに復帰運動すると、接点が離れ、遮断器が開
く。
Movement of the contacts 18 upward from the position shown in solid lines to the position shown in dashed lines engages the contacts and thus closes the circuit breaker, whereas a return movement downward disengages the contacts and opens the circuit breaker.

′作動棒18aが下側端蓋13内の開口を介して延
在し、可撓性の金属ベロー20が作動棒18aの周りの
真空対じとなり、外被10の内部の真空を損わずに作動
棒18aが垂直方向に移動出来るようにしている。
'The actuation rod 18a extends through an opening in the lower end cap 13, and a flexible metal bellows 20 provides a vacuum connection around the actuation rod 18a, without compromising the vacuum inside the jacket 10. The operating rod 18a is movable in the vertical direction.

第1図に示すように、金属ベロー20はその両端で作動
棒18a及び下側端蓋13に密封状態で固定されている
As shown in FIG. 1, the metal bellows 20 is fixed to the operating rod 18a and the lower end cover 13 at both ends thereof in a sealed manner.

各々の接点17及び18は略円形の円板の形であり、他
方の接点に向い合う1つの主面を持っている。
Each contact 17 and 18 is in the form of a generally circular disc and has one major surface facing the other contact.

各々の接点が、接点の他の部分に適当にろう付けされた
中心位置にあるボタン状接触部25を有する。
Each contact has a centrally located button-like contact portion 25 suitably brazed to the other portions of the contact.

各々のボタン状接触部がその中心位置に凹部27を持ち
、接点が第1図の破線で示す係合位置にある時、環状の
接触区域30でボタン状接触部の間の接触が起るように
なっている。
Each button-like contact has a recess 27 in its central position such that contact between the button-like contacts occurs in an annular contact area 30 when the contacts are in the engaged position shown in dashed lines in FIG. It has become.

この環状接触区域30は、閉じた接点を通る電流が、第
1図の鎖線で示すように、半径方向外向きに曲がるルー
プ状通路りをたどるような直径を持っている。
This annular contact area 30 has a diameter such that the current through the closed contact follows a loop-like path that bends radially outward, as shown in phantom in FIG.

このループ状通路りを流れる電流の磁気効果により、周
知のようにループが長くなる傾向がある。
The magnetic effect of the current flowing through this looped path tends to lengthen the loop, as is well known.

この結果、接点を分離して区域30の間にアークが形成
された時、ループを通る電流の磁気効果により、アーク
が半径方向外向きに追いやられる。
As a result, when the contacts are separated and an arc is formed between the areas 30, the magnetic effect of the current through the loop drives the arc radially outward.

半径方向外向きに作用する所望の強い力が得られるよう
に、このループ状通路のループを十分強める為、ボタン
状接触部25の外径は円板形接点の直径の半分より大き
くする。
In order to make the loop of this loop passage strong enough to obtain the desired strong radially outward force, the outer diameter of the button-shaped contact 25 is greater than half the diameter of the disc-shaped contact.

アークの末端が円板17及び18の外周に向って移動す
ると、アークは円周方向に作用する磁力を受け、この磁
力によってアークが円板の中心軸線の周りに回転する。
As the ends of the arc move towards the outer periphery of the discs 17 and 18, the arc is subjected to a magnetic force acting in the circumferential direction, which causes the arc to rotate about the central axis of the discs.

この円周方向に作用する磁力は、各々の円板に設けられ
且つ各々の円板を4つのフィンガ33に分割する4つの
溝孔32によって発生される。
This circumferentially acting magnetic force is generated by four slots 32 provided in each disc and dividing each disc into four fingers 33.

各々の溝孔32が、その円板17又は18の外周上の出
発点から、溝孔の中心線37がボタン状接触部25の外
周に対して略接線になるような通路をたどって、接点の
本体の中に入り込む。
Each slot 32 traces a path from its starting point on the outer periphery of its disk 17 or 18 such that the center line 37 of the slot is approximately tangent to the outer periphery of the button-shaped contact portion 25 to reach the contact point. into the body of.

中心線37が最初にボタン状接触部の周縁に接触する点
34を越えた位置まで、溝孔が一定の長さだけ引続いて
ボタン状接触部25の大体接線方向に伸びる。
The slot continues for a length generally tangentially to the button contact 25 beyond the point 34 where the centerline 37 first contacts the periphery of the button contact.

溝孔の接線方向に伸びる部分の一番内側の端に、半径方
向内向きに伸びる部分35があり、この部分35は接線
方向に伸びる部分に対して横方向に伸びる。
At the innermost end of the tangentially extending portion of the slot is a radially inwardly extending portion 35 which extends transversely to the tangentially extending portion.

この内向きに伸びる溝孔部分35がボタン状接触部25
の外周から、ボタン状接触部の外周より半径方向内側に
隔たる点36まで伸びる。
This inwardly extending slot portion 35 is the button-shaped contact portion 25.
from the outer periphery of the button contact portion to a point 36 spaced radially inwardly from the outer periphery of the button-like contact portion.

第2図に見られるように、ボタン状接触部が内向きに伸
びる溝孔部分35を横切り又は橋渡しをする。
As seen in FIG. 2, a button-like contact crosses or bridges the inwardly extending slot portion 35.

これらの溝孔32が、フィンガ33上のアーク末端へ又
はこのアーク末端から流れる電流に、アークの近辺で円
板の円周方向に伸びるフィンガ内の通路を強制的にたど
らせる。
These slots 32 force the current flowing to or from the arc end on the finger 33 to follow a path within the finger that extends circumferentially of the disk in the vicinity of the arc.

例えば、アーク末端が第2図の位置40にあるとすると
、フィンガ33を通ってアークに流れる電流の実効通路
は41に示すように、円板の円周方向に伸びる。
For example, if the arc end is at position 40 in FIG. 2, the effective path of current through the fingers 33 to the arc extends circumferentially around the disk, as shown at 41.

電流通路のこの円周方向の部分により、ループLを流れ
る電流が、アークを円板の中心軸線の周りに回転させる
円周方向に作用する正味の力成分を発生させる。
This circumferential portion of the current path causes the current flowing in loop L to generate a net force component acting in the circumferential direction that rotates the arc about the central axis of the disk.

円周方向に作用するこの力成分はアークの各々の末端を
フィンガ33の自由端で溝孔32を横切らせる程強く、
こうして接点の面上でアークの連続的な回転運動を生じ
させる。
This force component acting in the circumferential direction is strong enough to cause each end of the arc to traverse the slot 32 at the free end of the finger 33;
This creates a continuous rotational movement of the arc on the surface of the contact.

アークのこの連続的な回転運動が、アークによって発生
される金属蒸気の量を減らすことにより、大電流の遮断
を助け、こうして電流がゼロの時、金属蒸気が一層完全
に凝縮することが出来るようにする。
This continuous rotational motion of the arc helps interrupt large currents by reducing the amount of metal vapor produced by the arc, thus allowing the metal vapor to condense more completely when the current is zero. Make it.

アークによって発生された金属蒸気を凝縮させる為、適
当な蒸気凝縮用遮蔽体50及び54が設けられる。
Suitable vapor condensation shields 50 and 54 are provided to condense the metal vapor generated by the arc.

主遮蔽体50は接点17及び18を取巻く管状金属部材
であって、絶縁ケーシング11と接点間のアーク間隙と
の間に配置される。
The main shield 50 is a tubular metal member surrounding the contacts 17 and 18 and is located between the insulating casing 11 and the arc gap between the contacts.

この遮蔽体50は接点から電気的に隔離され、遮断器が
開いている時の2つの接点の電位の大体中間の電位に保
つことが好ましい。
This shield 50 is electrically isolated from the contacts and is preferably maintained at a potential approximately midway between the potentials of the two contacts when the circuit breaker is open.

この目的の為、ケーシング11の上半分及び下半分の間
に設けられ且つ密封されてケーシング11を通抜ける半
径方向のフランジ55により、遮蔽体がケーシング11
に支持される。
For this purpose, a shield is provided between the upper and lower halves of the casing 11 by means of a radial flange 55 which passes through the casing 11 in a sealed manner.
Supported by

夫々端蓋12及び13に接続された管状の補助遮蔽体5
4が主遮蔽体50の両端を取巻く。
Tubular auxiliary shields 5 connected to end caps 12 and 13, respectively
4 surrounds both ends of the main shield 50.

この補助遮蔽体は、とりわけ主遮蔽体を側路した蒸気を
凝縮させる作用がある。
This auxiliary shield serves, inter alia, to condense the steam that has bypassed the main shield.

小型にする為並びに経済性の為、管状の主遮蔽体50が
出来るだけ小さな直径を持つことが望ましい。
For reasons of compactness and economy, it is desirable for the tubular main shield 50 to have as small a diameter as possible.

同時に、接点17及び18が所定の大きさの電流を遮断
すべき場合、これらの接点が成る最低限の直径を持つこ
とが必要である。
At the same time, if the contacts 17 and 18 are to interrupt a certain amount of current, it is necessary that these contacts have a minimum diameter.

これらの2つの条件を充たすと、遮断器としては、接点
の外周と管状遮蔽体の内周との間に比較的小さなすき開
学間しか存在しなくなる。
When these two conditions are satisfied, the circuit breaker will have only a relatively small gap between the outer periphery of the contact and the inner periphery of the tubular shield.

例えば、非対称係数が1.3までで実効値が20000
アンペアの電流を遮断する定格の遮断器では、7.30
n(2にインチ)の直径を持つ接点と、10.16(J
(4インチ)の内径を持つ主遮蔽体とを用いるが、この
結果、接点と遮蔽体との間のすき開学間は僅か1.43
crrL(9/16インチ)になる。
For example, if the asymmetry coefficient is up to 1.3, the effective value is 20000.
For a circuit breaker rated to interrupt amps of current, 7.30
Contacts with a diameter of n (2 inches) and 10.16 (J
(4 inches) inside diameter, resulting in a contact-to-shield clearance of only 1.43 mm.
It becomes crrL (9/16 inch).

上に述べたような全体的な形並びに寸法の接点にこのよ
うな小さなすき開学間しかないと、大電流を遮断する際
、アークが遮蔽体の局部領域で過度の焼損及び溶融を生
ずるむしろ強い傾向があることが判った。
With such a small gap in the contacts of the overall shape and dimensions described above, when interrupting large currents, arcing can cause excessive burnout and melting of the shield in localized areas rather than It was found that there is a strong tendency.

明細書の初めに述べたように、発明者の研究によると、
この局部的な力ロ熱及び溶融の原因として考えられるの
は、接点の周縁上に、その領域のアークを半径方向外向
きに追いやる磁力成分がアークを円周方向に追いやる磁
力成分に較べて強い領域があることであることが判った
As stated at the beginning of the specification, according to the inventor's research,
A possible cause of this local force heating and melting is that the magnetic force component on the periphery of the contact point that drives the arc outward in the radial direction is stronger than the magnetic force component that drives the arc circumferentially. It turns out that there is an area.

半径方向外向きに作用するこの強い力成分により、アー
クが遮蔽体の内面に吹付けられ、この場所での遮蔽体の
壁の加熱及び侵食が増加する。
This strong force component acting radially outward causes an arc to be blown against the inner surface of the shield, increasing heating and erosion of the shield wall at this location.

遮蔽体材料の蒸発による圧力が高まると、アークの円周
方向の移動が阻害さn、その為遮蔽体の面のこの局部領
域に対する熱入力の割合が高くなる。
The increased pressure due to evaporation of the shield material impedes the circumferential movement of the arc, so that the rate of heat input to this local area of the face of the shield increases.

この為にアークが一層遅くなり、その結果この局部領域
に於ける遮蔽体の侵食が更に著しくなって、遮蔽体のこ
の局部領域に於ける加熱効果がピラミッド状に強まる。
This causes the arc to slow down more, resulting in more severe erosion of the shield in this local area and a pyramidal intensification of the heating effect in this local area of the shield.

差し当って第2図に示す形を持つ単一の接点を考えると
、アークに対し半径方向外向きに作用する磁力が、円周
方向に作用する力に較べて最も強いアークの位置は、円
周方向に伸びる各々のフィンガ33の根元の領域である
Considering for the moment a single contact having the shape shown in Figure 2, the location of the arc where the magnetic force acting radially outward on the arc is strongest compared to the force acting circumferentially is This is the region at the root of each finger 33 extending in the circumferential direction.

60に示すようなアークがこの特定の領域にあると、接
点を通ってアークに通ずる正味の電流通路62は殆んど
完全に半径方向であり、円周方向に伸びる成分が殆んど
或いは全くない。
With an arc such as that shown at 60 in this particular region, the net current path 62 through the contacts to the arc is almost entirely radial, with little or no circumferentially extending component. do not have.

この結果、通路62を電流が通ることによってこの領域
のアークに対して発生される主な力は、円周方向ではな
く半径方向であり、この結果、この領域のアークが隣接
した金属遮蔽体50に対して半径方向外向きにふき付け
られる強い傾向が生ずる。
As a result, the primary force exerted on the arc in this region by passing current through passageway 62 is radial rather than circumferential, with the result that the arc in this region There is a strong tendency to blow radially outward.

アークの末端が接点の円周方向にフィンガ33上へ移動
すれば、アークに対して円周方向に作用する力成分が半
径方向の力成分に対して漸進的に一層大きくなり、それ
に対応して、アークが遮蔽体に対して半径方向外向きに
ふき付けられる傾向が減少する。
If the end of the arc moves in the circumferential direction of the contact onto the finger 33, the force component acting on the arc in the circumferential direction becomes progressively larger with respect to the radial force component, and correspondingly , the tendency of the arc to be swept radially outwardly against the shield is reduced.

任意のフィンガ33の根元の領域にある間にアークが遮
蔽体50に対してふきとばされる傾向を少なくする為、
この発明では、2つの接点を互いに円周方向にずらし、
一方の接点に於ける溝孔32の出発点が他方の接点に於
ける溝孔の出発点から接点の周縁に沿って角度方向にず
れるようにする。
In order to reduce the tendency of the arc to be blown off against the shield 50 while in the region of the root of any finger 33,
In this invention, two contact points are shifted from each other in the circumferential direction,
The starting point of the slot 32 in one contact is angularly offset from the starting point of the slot in the other contact along the periphery of the contact.

この角度方向のずれが可能な最大限、即ち45°である
ことが好ましいカーこの発明はその広義の面では、35
°乃至55°のずれを考慮している。
Preferably, this angular deviation is the maximum possible, i.e. 45°.
A deviation of 55° is considered.

45°のずれが第3図に示されており、この場合、一方
の接点の溝孔32を実線で示し、他方の接点の溝孔を破
線で示しである。
A 45° offset is shown in FIG. 3, where the slots 32 in one contact are shown in solid lines and the slots in the other contact are shown in dashed lines.

このようにずらした結果、一方のアーク末端が、第3図
の70に示すように、一方の接点のフィンが33の根元
の、円周方向の力が弱い区域にある時、反対側のアーク
末端は他方の接点のフィンガ33上で十分光へ出た点に
あり、この為前記他方の接点はアークに対し円周方向に
作用する強い、駆動力を発生することが出来る。
As a result of this shift, when the fin of one contact is in the area of weak circumferential force at the root of 33, as shown at 70 in FIG. The distal end is at a sufficiently exposed point on the finger 33 of the other contact so that said other contact can generate a strong, driving force acting circumferentially on the arc.

接点の円周上の全ての点で、一方又は他方の接点がアー
クに対し円周方向に作用する強い力を発生することが出
来、この為、アークが占める周縁上の区域として、両方
の接点が円周方向に作用する弱い力及び半径方向外向き
に作用する強い力を発生するような区域はなくなる。
At every point on the circumference of the contacts, one or the other contact can generate a strong force acting circumferentially on the arc, so that as the area on the circumference occupied by the arc, both contacts There are no areas where the force exerts a weak force acting circumferentially and a strong force acting radially outward.

上に述べたように接点を角度方向に又は円周方向にずら
した結果、アークが接点の周縁領域に沿って移動する際
に、アークが過度に失速する傾向を持つような領域がな
くなる。
As a result of angularly or circumferentially offsetting the contacts as described above, there are no areas where the arc would have a tendency to stall excessively as it moves along the peripheral area of the contacts.

この結果、アークは接点の周縁に沿って一層溝らかに移
動し、この為遮蔽体に対しアーク・エネルギを一層一様
に分布させ、遮蔽体のどの局部領域でも過熱並びに過度
の蒸発の傾向が小さくなる。
As a result, the arc travels more smoothly along the periphery of the contact, thus distributing the arc energy more evenly to the shield, making any local area of the shield less susceptible to overheating and excessive evaporation. becomes smaller.

この発明は大電流遮断器(即ち非対称係数が13までソ
゛実効値16000アンペアより大きい電流を遮断する
定格であって、接点円板の直径が少なくても6.35C
rrL(2,5インチ)であることを必要とする遮断器
)に制限されることに注意され度い。
This invention is a high current circuit breaker (i.e., rated to interrupt currents greater than 16,000 amperes with an effective value of up to an asymmetry factor of 13, and having a contact disc diameter of at least 6.35C).
Please note that the circuit breaker is limited to rrL (2.5 inches).

前掲米国特許第3522399号に記載されるようなこ
れより低電流の遮断器では、遮蔽体と接点とのすき間を
典型的な値にした場合、2つの接点の溝孔の出発点を角
度方向にずらすことにより、遮蔽体の局部的な溶融は目
立って減少することがない、前掲特許に記載される形の
遮断器で商業的に使われるものは、接点円板の直径が僅
か約3.49cWL(13/8インチ)であり、遮蔽体
と接点とのすき間が約1、o 3crrL(13/32
インチ)であり、遮断定格は典型的な最大非対称係数の
場合で実効値60000アンペアである。
In lower current circuit breakers, such as those described in U.S. Pat. Localized melting of the shield is not appreciably reduced by shifting, and circuit breakers of the type described in the above-cited patent, used commercially, have contact disc diameters of only about 3.49 cWL. (13/8 inch), and the gap between the shield and the contact is approximately 1, o 3 crrL (13/32 inch).
inches), and the interrupting rating is 60,000 amps rms at typical maximum asymmetry factors.

この発明の好ましい形式では、各々の溝孔32を直ぐ隣
接したフィンガ33の平均の幅に較べて比較的幅広くし
て、フィンガを通ってその上のアーク末端へ流れる電流
を更に円周方向に近い向きの通路に集中し、こうしてこ
の通路を通る電流により発生される磁力の円周方向に作
用する成分を強める。
In a preferred form of the invention, each slot 32 is made relatively wide compared to the average width of immediately adjacent fingers 33 to direct the current flowing through the finger to the arc end thereon in a more nearly circumferential direction. oriented path, thus strengthening the circumferentially acting component of the magnetic force generated by the current passing through this path.

この方針に沿って、溝孔の平均の幅は、フィンガが円板
の円周と平行に伸びる領域で考えて、フィンガの平均の
幅の1/3より大きくすることが好ましい。
Along this line, the average width of the slots is preferably greater than 1/3 of the average width of the fingers, considered in the area where the fingers extend parallel to the circumference of the disc.

これらの幅は他方の接点から第2図で見たようにして測
った幅である。
These widths are measured from the other contact point as seen in FIG.

この発明の特定の実施例を図示し且つ説明したが、この
発明の範囲内で種々の変更が可能であることは当業者に
明らかであろう。
While specific embodiments of the invention have been illustrated and described, it will be obvious to those skilled in the art that various modifications may be made within the scope of the invention.

従って、これら全ての変更は、特許請求の範囲の記載に
合致する限り、この発明の範囲内に属すると承知され度
い。
Therefore, all such modifications are deemed to fall within the scope of this invention as long as they are consistent with the scope of the claims.

この発明は特許請求の範囲の記載に関連して次の実態様
を取り得る。
This invention can take the following embodiments in relation to the claims.

@)接点の外周と遮蔽体の内周との間で測ったすき開学
間の幅が1.59cIrL(5/8インチ)以下である
こと。
@) The width of the gap measured between the outer circumference of the contact and the inner circumference of the shield is 1.59 cIrL (5/8 inch) or less.

(D)円板形の両接点が略同じ直径を持ち、大体円形の
その周縁が半径方向に実質的に整合していること。
(D) Both disc-shaped contacts have substantially the same diameter and their generally circular peripheries are substantially aligned in the radial direction.

(ハ)各々の接点がその外周で、円周方向に伸びるフィ
ンガ部分の根元に、アーク末端が占め得る領域を持ち、
該領域に対して電流が接点の中心部分から、実質的に接
線成分を持たずに略完全に半径方向である通路に沿って
流れることが出来、この為電流が前記通路を通過する際
、前記領域の1つにその末端を持つアークに対し主に半
径方向外向きに作用する力を発生させること。
(c) Each contact point has an area on its outer periphery, which can be occupied by an arc end, at the root of a circumferentially extending finger portion;
For said region, current can flow from the central portion of the contact along a path that is substantially entirely radial, with substantially no tangential component, so that as the current passes through said path, said Generating a force acting primarily radially outward on an arc having its terminus in one of the regions.

に)前記(ハ)項に於て、一方の接点にあるフィンガ部
分の根元に於ける前記領域が他方の接点に於ける前記領
域から角度方向に35乃至55°ずれていること。
B) In the above item (C), the area at the root of the finger portion at one contact point is angularly offset by 35 to 55 degrees from the area at the other contact point.

(ホ)接点の角度方向のずれが約45°であると。(E) The angular deviation of the contact points is approximately 45°.

(へ)各接点の幅を他方の接点から見た場合で測って、
各々の溝孔の接線部分の平均の幅が該溝孔に直ぐ隣接す
るフィンガ部分の平均の幅の%より大きいこと。
(f) Measure the width of each contact when viewed from the other contact,
The average width of the tangential portion of each slot is greater than a percentage of the average width of the finger portions immediately adjacent to the slot.

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

第1図はこの発明の1形式を実施した真空遮断器の一部
分を断面で示す側面図、第2図は第1図の線2−2で切
った平面図、第3図は第1図の矢印3の方向に見た遮断
器の成る部分の略図である。 主な符号の説明、10:外被、17,18:円板形接点
、25:ホモン状接触部、32:溝孔、33:フィンガ
、35:半径方向内向きに伸びる部分、37:中心線、
50,54:遮蔽体。
FIG. 1 is a side view showing a section of a part of a vacuum circuit breaker implementing one type of the present invention, FIG. 2 is a plan view taken along line 2--2 in FIG. 1, and FIG. 3 is a schematic view of the parts of the circuit breaker viewed in the direction of arrow 3; FIG. Explanation of main symbols, 10: Outer cover, 17, 18: Disc-shaped contact, 25: Homonic contact part, 32: Slot, 33: Finger, 35: Portion extending radially inward, 37: Center line ,
50, 54: Shielding body.

Claims (1)

【特許請求の範囲】[Claims] 1 非対称係数が1.3までの実効値16000アンペ
アより大きな電流を遮断する真空遮断器に於て、10=
トル以下の圧力まで真空にされた外被と、該外被内にあ
る相対的に可動の1対の円板形接点と、前記円板形接点
を取巻き且つ遮断器が開いている時、それから電気的に
隔離されている管状金属遮蔽体とを有し、各々の接点は
直径が6,351(2,5インチ)より大きく、大体円
形の外周を持つと共に、他方の接点に向い合っていて該
他方の接点と係合し得る接触面を持ち、各々の接点はそ
の接触面に中心の近くで前記円板形接点の外周と略同心
の略円形の外周を持つボタン状接触部を持ち、該ボタン
状接触部の直径が前記円板形接点の直径の半分より大き
く、該ボタン状接触部は遮断器が閉じている時相互に接
触し、遮断器が離れる時アークが開始される領域を構成
し、前記円板形接点は直径が大きいのでボタン状接触部
から接点外周部にアークを半径方向外向きに1駆動する
半径方向外向き作用の磁力をアークに生じ、且つその後
膣アークを前記遮蔽体に向けて半径方向外向きにふき付
ける様に作用し、各々の接点は円周方向に相隔たる4つ
の溝孔を持ち、各々の溝孔は接点の外周上の出発点から
、溝孔の中心線領域が前記ボタン状接触部の外周に対し
て大体接線方向であるような通路をたどって接点の本体
に入り込む接線部分を持ち、こうして接点の外周と溝孔
の接線部分の間に円周方向に伸びるフィンガ部分を構成
し、各々の接点がその外周で、円周方向に伸びるフィン
ガ部分の根元に、アーク末端が占め得る領域を持ち、該
領域に対して電流が接点の中心部分から、実質的に接線
成分を持たずに略完全に半径方向である通路に沿って流
れることが出来、この為電流が前記通路を通過する際、
前記領域の1つにその末端を持つアークに対し主に半径
方向外向きに作用する磁力を発生させ、各々の溝孔は前
記接線部分の一番内側の端に、該接線部分の横方向に且
つ接点の本体の半径方向内向きに、前記ボタン状接触部
の外周より半径方向内側に隔たる点まで伸びる部分を有
し、前記遮蔽体の内周が円板形接点の外周から小さな環
状すき開学間によって隔てられ、各々の接点に於ける溝
孔の出発点が接点の外周に沿って略等間隔であり、前記
接点が互いに角度方向にずらされていて、一方の接点の
溝孔の出発点が他方の接点の溝孔の出発点から接点の周
縁に沿って35°乃至55°ずらされるようにした真空
遮断器。
1 In a vacuum circuit breaker that interrupts a current larger than an effective value of 16,000 amperes with an asymmetry factor of up to 1.3, 10=
a housing evacuated to a pressure below Torr; a pair of relatively movable disc-shaped contacts within the housing; and a pair of disc-shaped contacts surrounding said disc-shaped contacts and when the circuit breaker is open; an electrically isolated tubular metal shield, each contact having a diameter greater than 6,351 (2.5 inches), having a generally circular outer circumference, and facing the other contact; each contact has a contact surface capable of engaging with the other contact, each contact having a button-shaped contact portion on the contact surface having a substantially circular outer periphery substantially concentric with the outer periphery of the disc-shaped contact near the center; The diameter of the button-shaped contacts is larger than half the diameter of the disk-shaped contacts, and the button-shaped contacts contact each other when the circuit breaker is closed, and define an area where an arc is initiated when the circuit breaker is released. Since the disc-shaped contact has a large diameter, it produces a radially outward magnetic force on the arc that drives the arc radially outward from the button-shaped contact portion to the outer periphery of the contact, and then causes the vaginal arc to Acting to spray radially outward toward the shield, each contact has four circumferentially spaced slots, each slot extending from its starting point on the outer periphery of the contact to the slot. has a tangential portion that enters the body of the contact following a path such that the centerline area of the button is generally tangential to the outer periphery of the button-shaped contact, thus forming a circle between the outer periphery of the contact and the tangential portion of the slot. comprising circumferentially extending finger portions, each contact having at its outer periphery, at the root of the circumferentially extending finger portion, an area that can be occupied by an arc end, to which area the current is directed from the central portion of the contact. , can flow along a path that is substantially completely radial without having a substantially tangential component, so that when the current passes through said path,
generating a magnetic force acting primarily radially outward on an arc having its terminus in one of said regions, each slot having a slot at the innermost end of said tangential section, transversely of said tangential section; and a portion extending radially inward of the main body of the contact to a point spaced radially inward from the outer periphery of the button-shaped contact portion, and the inner periphery of the shield has a small annular gap from the outer periphery of the disc-shaped contact. separated by apertures, the starting points of the slots in each contact are substantially equally spaced along the outer circumference of the contacts, and the contacts are angularly offset from each other such that the starting points of the slots in one contact A vacuum circuit breaker in which the starting point is offset from the starting point of the slot of the other contact by 35° to 55° along the periphery of the contact.
JP48142569A 1972-12-21 1973-12-21 vacuum circuit breaker Expired JPS5938688B2 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US00317222A US3809836A (en) 1972-12-21 1972-12-21 Vacuum-type electric circuit interrupter
US317222 1989-02-28

Publications (2)

Publication Number Publication Date
JPS4996271A JPS4996271A (en) 1974-09-12
JPS5938688B2 true JPS5938688B2 (en) 1984-09-18

Family

ID=23232670

Family Applications (1)

Application Number Title Priority Date Filing Date
JP48142569A Expired JPS5938688B2 (en) 1972-12-21 1973-12-21 vacuum circuit breaker

Country Status (6)

Country Link
US (1) US3809836A (en)
JP (1) JPS5938688B2 (en)
CA (1) CA959524A (en)
DE (1) DE2363044C2 (en)
FR (1) FR2211737B1 (en)
GB (1) GB1432060A (en)

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Also Published As

Publication number Publication date
GB1432060A (en) 1976-04-14
FR2211737B1 (en) 1980-05-23
JPS4996271A (en) 1974-09-12
DE2363044A1 (en) 1974-07-04
DE2363044C2 (en) 1983-03-03
FR2211737A1 (en) 1974-07-19
CA959524A (en) 1974-12-17
US3809836A (en) 1974-05-07

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