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JPH0693340B2 - Vacuum interrupter electrode material - Google Patents
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JPH0693340B2 - Vacuum interrupter electrode material - Google Patents

Vacuum interrupter electrode material

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Publication number
JPH0693340B2
JPH0693340B2 JP6016186A JP6016186A JPH0693340B2 JP H0693340 B2 JPH0693340 B2 JP H0693340B2 JP 6016186 A JP6016186 A JP 6016186A JP 6016186 A JP6016186 A JP 6016186A JP H0693340 B2 JPH0693340 B2 JP H0693340B2
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Japan
Prior art keywords
electrode material
vacuum interrupter
electrode
vacuum
less
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
Application number
JP6016186A
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Japanese (ja)
Other versions
JPS62217519A (en
Inventor
佳行 柏木
Original Assignee
株式会社明電舍
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Priority to JP6016186A priority Critical patent/JPH0693340B2/en
Publication of JPS62217519A publication Critical patent/JPS62217519A/en
Publication of JPH0693340B2 publication Critical patent/JPH0693340B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 A.産業上の利用分野 本発明は、真空インタラプタの電極材料に関する。The present invention relates to a vacuum interrupter electrode material.

B.発明の概要 本発明は、銅,モリブデンおよびクロムからなる合金に
より形成した真空インタラプタの電極材料において、 電極材料を、銅55〜80重量%,モリブデン15〜35重量%
およびクロム4〜12重量%の合金により形成し、モリブ
デンおよびクロム粉末の粒径を限定することにより、 閃絡(再点弧,再発弧)の確率が極めて低く、特に多頻
度開閉が可能であつてコンデンサ開閉用として最適とし
たものである。
B. Outline of the Invention The present invention relates to a vacuum interrupter electrode material formed of an alloy composed of copper, molybdenum and chromium, wherein the electrode material is 55 to 80% by weight of copper and 15 to 35% by weight of molybdenum.
And chromium 4 to 12% by weight, and by limiting the particle size of the molybdenum and chromium powders, the probability of flashover (re-ignition, re-ignition) is extremely low, and frequent opening and closing is possible. It is the most suitable for opening and closing capacitors.

C.従来の技術 一般に、真空インタラプタの電極材料は、 大電流をしや断する能力が高いこと、 絶縁耐力が高いこと、 耐溶着性が良好なこと、 小電流を良好にしや断できること、 等の条件を満足することが要求されている。C. Conventional technology Generally, the electrode material of a vacuum interrupter has a high ability to cut or cut a large current, a high dielectric strength, a good welding resistance, a small current can be cut or cut, etc. Is required to be satisfied.

従来、上記条件を満足するものとして、例えば特開昭59
−27418号公報に開示される電極材料が知られている。
かかる真空インタラプタの電極材料は、粒径がそれぞれ
同じ149μm以下(−100メツシユ)のモリブデンMoおよ
びクロムCrの粉末を焼結して焼結体を形成し、この焼結
体に銅Cuを溶浸したCu20〜70重量%,Mo10〜70重量%お
よびCr10〜70重量%の合金からなつている。
Conventionally, as one satisfying the above conditions, for example, Japanese Patent Laid-Open No.
The electrode material disclosed in Japanese Patent No. 27418 is known.
The electrode material of such a vacuum interrupter is obtained by sintering powders of molybdenum Mo and chromium Cr having the same grain size of 149 μm or less (-100 mesh) to form a sintered body, and infiltrating copper Cu into the sintered body. The alloy is composed of 20 to 70 wt% Cu, 10 to 70 wt% Mo and 10 to 70 wt% Cr.

D.発明が解決しようとする問題点 上記従来の真空インタラプタの電極材料は、優れたしや
断性能を有し、特に事故大電流しや断に優れ、高耐電圧
特性を示す。
D. Problems to be Solved by the Invention The electrode material of the conventional vacuum interrupter described above has excellent breaking and breaking performance, is particularly excellent in breaking and breaking a large current due to an accident, and exhibits high withstand voltage characteristics.

しかし、この真空インタラプタの電極材料を用いてコン
デンサ開閉を行つたところ、再点弧の発生が見られた。
コンデンサ開閉の場合は、通常の開閉と異なり、開極時
に系統電圧の2倍の電圧が極間にかかり、また投入時に
は系統電流の5倍程度の瞬時大電流(ラツシユカレン
ト)が流れる。このため、開閉が多頻度のコンデンサ開
閉においては、再点弧,再発弧を起こし易いので、開閉
を確実に行わないと回路を破壊させてしまう虞れがあ
る。
However, when a capacitor was opened and closed using the electrode material of this vacuum interrupter, reignition occurred.
In the case of opening and closing the capacitor, unlike normal switching, a voltage twice as high as the system voltage is applied between the electrodes at the time of opening, and an instantaneous large current (rush current) of about 5 times as much as the system current flows when the capacitor is turned on. For this reason, when the capacitor is frequently opened and closed, re-ignition and re-ignition are likely to occur, so that the circuit may be destroyed unless the opening and closing is performed reliably.

再点弧,再発弧現象を防止するためには、一つとして電
極材料における酸化物,ガス不純物,ピンホール等の不
安定要素を無くすことが必要である。
In order to prevent re-ignition and re-ignition, it is necessary to eliminate unstable elements such as oxides, gas impurities and pinholes in the electrode material.

ところで、Cu−Mo−Cr合金の多孔質基材(スケルトン)
となるMo−Cr焼結体において、Crは酸化し易く、Cr粒子
の表面に不動態膜が形成され易い。このため、Crの量が
多いと、Cr粒子表面の不動態膜の存在によつてCuの漏れ
性が悪くなり、空孔,溶浸欠陥ができ、ピンホールを作
る傾向が顕著となつて、再点弧,再発弧現象を生じ易く
なる。一方、Crの量を少なくすると、Moの量を多くしな
ければならないが、Moは熱電子を放出し易い傾向にある
ため、Moをあまり多量に使用すると耐電圧特性を低下さ
せることになつてしまう。
By the way, Cu-Mo-Cr alloy porous substrate (skeleton)
In the Mo-Cr sintered body as described below, Cr is easily oxidized and a passivation film is easily formed on the surface of Cr particles. Therefore, when the amount of Cr is large, the leaking property of Cu deteriorates due to the presence of the passivation film on the surface of the Cr particles, and voids and infiltration defects are generated, and the tendency to form pinholes becomes remarkable. Re-ignition and re-ignition phenomena are likely to occur. On the other hand, if the amount of Cr is reduced, the amount of Mo must be increased, but since Mo tends to emit thermoelectrons, use of too much Mo leads to deterioration in withstand voltage characteristics. I will end up.

そこで、発明者は、上記従来のCu−Mo−Cr合金におい
て、合金製造前におけるMoおよびCr粉末の最大粒径が共
に149μm(−100メツシユ)であるという点に着目し、
MoおよびCr粉末の最大粒径を異なつたものにさせること
により、両者の拡散結合を確実に行い、Mo−Cr焼結体に
おいて、Mo,Crの各粒子がそれぞれ単独で存在する割合
を少なくしようとしたのである。なぜならば、Mo,Crの
各粒子(Moの粉末同志,Cr粉末同志が結合して大きくな
つている粒子も含む)が単独で存在し、その粒子に直接
アークスポツトができると、MoおよびCrのそれぞれの欠
点が顕著に現われてしまうからである。
Then, the inventor paid attention to the fact that in the above-mentioned conventional Cu-Mo-Cr alloy, both the maximum particle diameters of Mo and Cr powders before the alloy production were 149 µm (-100 mesh),
By making the maximum particle diameters of Mo and Cr powders different from each other, diffusion bonding between them can be surely performed, and in the Mo-Cr sintered body, it is possible to reduce the proportion of each particle of Mo and Cr existing independently. It was. Because each of Mo and Cr particles (including particles of Mo powder and particles of Cr powder that are combined and growing) is present independently, and if an arc spot is directly formed on that particle, the particles of Mo and Cr This is because each of these drawbacks will appear prominently.

E.問題点を解決するための手段 上記従来の問題点を解決するために、本発明は、Mo粉末
とCr粉末とからなる多孔質基材の空隙を銅で満たしてな
る真空インタラプタの電極材料において、Cu55〜80重量
%,Mo15〜35重量%およびCr4〜12重量%の合金からな
り、合金製造前におけるCrの粒径が149μm以下、Moの
最大粒径がCrの最大粒径の1/2以下としたものである。
E. Means for Solving Problems In order to solve the above-mentioned conventional problems, the present invention provides an electrode material for a vacuum interrupter in which the voids of a porous base material composed of Mo powder and Cr powder are filled with copper. In, the alloy consists of 55-80% by weight of Cu, 15-35% by weight of Mo and 4-12% by weight of Cr, the grain size of Cr before alloy production is 149 μm or less, and the maximum grain size of Mo is 1 / the maximum grain size of Cr. It is set to 2 or less.

Cuが55重量%未満の場合には、導電率が低下するととも
に接触抵抗が大きくなつてしまい、80重量%を越える場
合には、耐溶着性が悪化してしまう。また、Moが15重量
%未満の場合には、耐溶着性が悪化し、35重量%を越え
る場合には、閃絡の確率が高くなるとともに電流しや断
能力が低下してしまう。さらに、Crが4重量%未満の場
合には、再点弧の確率が高くなるとともに耐溶着性が悪
化してしまい、12重量%を越える場合には、閃絡の確率
が高くなつてしまう。
If the Cu content is less than 55% by weight, the electrical conductivity will decrease and the contact resistance will increase, and if it exceeds 80% by weight, the welding resistance will deteriorate. Further, when Mo is less than 15% by weight, the welding resistance is deteriorated, and when it exceeds 35% by weight, the probability of flashover becomes high and the current-carrying ability and the disconnecting ability are deteriorated. Further, when Cr is less than 4% by weight, the probability of re-ignition increases and the welding resistance deteriorates, and when it exceeds 12% by weight, the probability of flashover increases.

F.作用 かかる構成の真空インタラプタの電極材料においては、
Crに対してMoの粒径は小さく、かつCrに対してMoの量を
多くしているので、MoとCrとが十分に拡散結合して多孔
質基材の焼結体を形成しており、Mo,Crがそれぞれ単独
で存在する割合が極めて少なくなつて、MoまたはCrの粒
子上に直接アークスポツトができなくなるものと考えら
れる。また、Crの量が少ないので、Cr粒子表面の不動態
膜の悪影響もなくなり、しかも、Moと拡散結合する際に
一部は放出除去されて一層不動態膜の悪影響がなくなる
ものと考えられる。これにより、本発明の真空インタラ
プタの電極材料によれば、閃絡(再点弧,再発弧)の発
生率が極めて少なくなり、安定して多頻度の開閉が行わ
れる。
F. Action In the electrode material of the vacuum interrupter having such a configuration,
Since the grain size of Mo is smaller than that of Cr and the amount of Mo is larger than that of Cr, Mo and Cr are sufficiently diffusion-bonded to form a sintered body of a porous substrate. It is considered that the arc spots cannot be directly formed on the particles of Mo or Cr because the proportions of Mo, Cr and Cr present respectively are extremely small. Further, since the amount of Cr is small, it is considered that the adverse effect of the passivation film on the surface of the Cr particles is eliminated, and further, a part thereof is released and removed when diffusion-bonding with Mo, and the adverse effect of the passivation film is further eliminated. Therefore, according to the electrode material of the vacuum interrupter of the present invention, the occurrence rate of flashover (re-ignition, re-arcing) is extremely reduced, and stable frequent opening and closing is performed.

G.実施例 以下、本発明を図に示す一実施例に基づき詳細に説明す
る。
G. Example Hereinafter, the present invention will be described in detail based on an example shown in the drawings.

本発明に係る電極材料を用いた真空インタラプタは、例
えば第3図に示すように、真空容器1内にその軸線上に
位置せしめて1対の電極棒2,2を相対的に接近離反自在
に導入し、各電極棒2の内端部に対をなす電極3,3を絶
縁スペーサを介在せしめて固着し、各電極棒2と電極3
とを、電極3の背部に配設されかつ電極棒2に流れる軸
方向(第3図において上下方向)の電流を電極棒2を中
心とするループ電流に変更して縦磁界を発生する磁界発
生部材であるコイル4,4により接続して概略構成されて
いる。
A vacuum interrupter using the electrode material according to the present invention is, for example, as shown in FIG. 3, positioned in the vacuum container 1 on its axis so that a pair of electrode rods 2, 2 can be relatively moved toward and away from each other. Introduced, the electrodes 3, 3 forming a pair are fixed to the inner end portion of each electrode rod 2 with an insulating spacer interposed, and each electrode rod 2 and electrode 3 is fixed.
Are generated on the back side of the electrode 3 and change the axial current (vertical direction in FIG. 3) flowing through the electrode rod 2 into a loop current centered on the electrode rod 2 to generate a longitudinal magnetic field. The coils 4 and 4 as members are connected to each other to have a schematic structure.

すなわち、真空容器1は、ガラスまたはセラミツクスか
らなる円筒状の2本の絶縁筒5,5を両端に固着したFe−N
i−Co合金、またはFe−Ni合金等からなる薄肉円環状の
封着金具6,6…の一方を介し接合して1本の絶縁筒とす
るとともに、その両開口端を他方の封着金具6,6を介し
円板状の金属端板7,7により閉塞し、かつ内部を高真空
(たとえば6.665mPa以下の圧力)に排気して形成されて
いる。そして、真空容器1内には、前記各電極棒2がそ
れぞれの金属端板7の中央から真空容器1の気密性を保
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 container 1 is made of Fe-N in which two cylindrical insulating cylinders 5 made of glass or ceramics are fixed at both ends.
Thin-walled ring-shaped sealing metal fittings 6, 6 made of i-Co alloy or Fe-Ni alloy, etc. are joined together to form one insulating cylinder, and both open ends of the other sealing metal fittings. It is formed by closing the disc-shaped metal end plates 7 and 7 via 6 and 6, and evacuating the inside to a high vacuum (for example, a pressure of 6.665 mPa or less). Then, the electrode rods 2 are introduced into the vacuum container 1 from the center of the respective metal end plates 7 so as to be relatively close to and away from each other while maintaining the airtightness of the vacuum container 1.

なお、一方(第3図において上方)の電極棒2は、一方
の金属端板7に気密に挿着されているものであり、他方
の電極棒2は、金属ベローズ8を介し真空容器1の気密
性を保持して他方の金属端板7を軸方向へ移動自在に挿
通されているものである。また、第3図において9およ
び10は軸シールドおよびベローズシールド、11は主シー
ルド、12は補助シールドである。
One of the electrode rods 2 (upper side in FIG. 3) is airtightly attached to one of the metal end plates 7, and the other electrode rod 2 of the vacuum container 1 has a metal bellows 8 interposed therebetween. The other metal end plate 7 is inserted movably in the axial direction while maintaining airtightness. In FIG. 3, 9 and 10 are shaft shields and bellows shields, 11 is a main shield, and 12 is an auxiliary shield.

前記各電極棒2の内端部には、第1図および第2図に示
すように、Cuの如く高導電率の材料からなるとともに、
電極棒2の直径より適宜大径の円板状の取付ベース4a
と、取付ベース4aの外周の相対する位置から半径方向
(第1図において左右方向)外方へ延在する2本のアー
ム4bと、各アーム4bの端部から取付ベース4aを中心とし
て同一方向へ円弧状に彎曲した円弧部4cとからなる1/2
分流タイプのコイル4が、取付ベース4aの一方(第1図
において下方)の面に形成した凹部13を介しろう付によ
り固着されている。
As shown in FIGS. 1 and 2, the inner end portion of each electrode rod 2 is made of a material having high conductivity such as Cu, and
Disc-shaped mounting base 4a with a diameter appropriately larger than the diameter of the electrode rod 2
And two arms 4b extending outward in the radial direction (left-right direction in FIG. 1) from opposite positions on the outer circumference of the mounting base 4a, and in the same direction from the end of each arm 4b about the mounting base 4a. 1/2 consisting of a circular arc part 4c curved in a circular arc shape
The shunt type coil 4 is fixed by brazing via a recess 13 formed on one surface (downward in FIG. 1) of the mounting base 4a.

そして、コイル4は、電極棒2の内端外周にろう付によ
り嵌着したリング状の取付部14aと、取付部14aの外周か
ら半径方向外方へ放射状に延伸した複数の支持腕14b
と、各支持腕14bの端部を連結するリング状の支持部14c
とからなるコイル補強体14とろう付されて補強されてい
る。
The coil 4 includes a ring-shaped mounting portion 14a fitted to the outer periphery of the inner end of the electrode rod 2 by brazing, and a plurality of support arms 14b radially extending outward from the outer periphery of the mounting portion 14a.
And a ring-shaped support portion 14c that connects the ends of the support arms 14b.
And a coil reinforcing member 14 made of and are brazed and reinforced.

なお、コイル補強体14は、ステンレス鋼の如く機械的強
度大にしてかつ低導電率の材料からなるものである。
The coil reinforcement 14 is made of a material having high mechanical strength and low electrical conductivity such as stainless steel.

前記コイル4の取付ベース4aの他方の面には、円形の凹
部15が設けられており、この凹部15には、ステンレス鋼
またはインコネルの如く機械的強度大にしてかつ低導電
率の材料により短円筒状に形成した絶縁スペーサ16が、
その一端に形成した小径フランジ16aを介しろう付によ
り固着されている。そして、絶縁スペーサ16の他端に形
成した大径フランジ16bには、この大径フランジ16bより
適宜大径にしてかつ絶縁スペーサ16の内径とほぼ同径の
透孔を有する円輪板状の取付ベース17aと、取付ベース1
7aの外周の相対する位置から半径方向外方へ延在した2
本のアーム17bと、各アーム17bの端部からコイル4の円
弧部4cとほぼ等しい曲率半径にしてかつこれとは逆の同
一方向へ適宜の長さで円弧状に彎曲した円弧部17cとか
らなり、銅の如く高導電率の材料により形成された補助
コイル17が、取付ベース17aの一方(第2図において下
方)の面に設けた係合段部18を介しろう付により固着さ
れている。そして、補助コイル17とコイル4とは、補助
コイル17の各円弧部17cの端部に設けた凹部19に一端を
固着し、かつ他端をコイル4の各円弧部4cの端部に設け
た透孔21に挿着した軸方向の通電ピン20を介し電気的に
接続されている。
A circular recess 15 is provided on the other surface of the mounting base 4a of the coil 4, and the recess 15 is made of a material such as stainless steel or Inconel having high mechanical strength and low conductivity. The insulating spacer 16 formed in a cylindrical shape,
It is fixed by brazing via a small diameter flange 16a formed at one end thereof. Then, the large-diameter flange 16b formed on the other end of the insulating spacer 16 is mounted in the shape of a circular plate having a through hole having a diameter substantially larger than that of the large-diameter flange 16b and having a diameter substantially equal to the inner diameter of the insulating spacer 16. Base 17a and mounting base 1
2 extending outward in the radial direction from opposite positions on the outer circumference of 7a
From the arm 17b of the book and the arc portion 17c which has a radius of curvature substantially equal to that of the arc portion 4c of the coil 4 from the end of each arm 17b and which is curved in an arc shape with an appropriate length in the same direction opposite to this. The auxiliary coil 17 made of a material having high conductivity such as copper is fixed by brazing via the engaging step portion 18 provided on one surface (downward in FIG. 2) of the mounting base 17a. . The auxiliary coil 17 and the coil 4 have one end fixed to a recess 19 provided at the end of each arc portion 17c of the auxiliary coil 17, and the other end provided at the end of each arc portion 4c of the coil 4. It is electrically connected via an axial current-carrying pin 20 inserted into the through hole 21.

補助コイル17には、コイル4の直径とほぼ同径(外径80
mm)に形成した電極3が、その背面中央に設けた凹部21
を介しろう付により取付ベース17aと接合されるととも
に、背面を介しろう付により各アーム17bおよび円弧部1
7cと接合されている。電極3の対向面は、Cu60重量%、
Mo30重量%およびCr10重量%の合金からなる円板状の薄
板22で形成されている。薄板22の中央部には、外径30mm
の円板状に突出して対向電極と接離自在の接触部23が設
けられており、接触部23より径大の部分は、アーク拡散
部24となつている。本実施例において、接触部23の板厚
は2mm,アーク拡散部24の板厚は1mmにそれぞれ形成され
ている。
The diameter of the auxiliary coil 17 is approximately the same as the diameter of the coil 4 (outer diameter 80
mm) electrode 3 has a recess 21 formed in the center of the back surface thereof.
It is joined to the mounting base 17a by brazing via each of the arms, and each arm 17b and the arc portion 1 are also brazed via the back surface.
It is joined with 7c. The facing surface of the electrode 3 is 60% by weight of Cu,
It is formed of a disc-shaped thin plate 22 made of an alloy of Mo 30% by weight and Cr 10% by weight. The outer diameter of the thin plate 22 is 30 mm in the center.
Is provided with a contact portion 23 protruding in a disk shape and capable of coming into contact with and separating from the counter electrode, and a portion having a diameter larger than the contact portion 23 serves as an arc diffusion portion 24. In this embodiment, the contact portion 23 has a thickness of 2 mm and the arc diffusion portion 24 has a thickness of 1 mm.

一方、電極3の対向面以外(薄板22以外)の部分である
背面部25は、導電率(IACS%)が7%の40Cu−20Cr−40
Feにより形成されている。薄板22と背面部25とは、ろう
付接合するか、または薄板22のCuを溶浸させる際に同時
に背面部25を接合する。
On the other hand, the back surface portion 25, which is a portion other than the facing surface of the electrode 3 (other than the thin plate 22), has a conductivity (IACS%) of 7% of 40Cu-20Cr-40.
It is made of Fe. The thin plate 22 and the back surface part 25 are joined by brazing or the back surface part 25 is joined at the same time when Cu of the thin plate 22 is infiltrated.

前記電極3の薄板22を形成する電極材料を製造するに
は、最大粒径74μm以下でかつ平均粒径3μmのMo粉末
と粒径が149μm以下(−100メツシユ)のCr粉末を、所
定量機械的に混合するとともに、この混合粉末をアルミ
ナ容器に収納し、その混合粉末上にCuのブロツクを載置
する。そして、これらを6.67mPa以下の圧力に保持した
真空炉中にて、1000℃で10分間加熱し、Mo−Crの焼結体
(多孔質基材)を形成する。次に、真空炉を1150℃に昇
温して10分間加熱し、その後炉冷固化することにより電
極材料が製造される。
In order to manufacture the electrode material for forming the thin plate 22 of the electrode 3, a predetermined amount of Mo powder having a maximum particle size of 74 μm or less and an average particle size of 3 μm and Cr powder having a particle size of 149 μm or less (-100 mesh) are machined. The mixed powder is stored in an alumina container, and a Cu block is placed on the mixed powder. Then, these are heated at 1000 ° C. for 10 minutes in a vacuum furnace maintained at a pressure of 6.67 mPa or less to form a Mo—Cr sintered body (porous substrate). Next, the vacuum furnace is heated to 1150 ° C., heated for 10 minutes, and then cooled and solidified in the furnace to manufacture an electrode material.

上記構成の真空インタラプタをコンデンサ開閉として回
路に組込み、閃絡確率を調べた。試験方法は、66kV−60
MVAのコンデンサ容量の開閉条件と等価となるようにし
た。投入条件は、予めコンデンサに直流電圧54kVr.m.s.
を充電し、LC振動により3700Aピーク,200サイクルの電
流を流した。一方、しや断は、50サイクル電源電圧50kV
r.m.s.,電流520Aの進相電流とし、この条件で投入しや
断を多数回繰り返した。また、極間ギヤツプは15mm,投
入スピードは1m/sec,しや断スピードは2m/secである。
その結果を次表および第4図に示した。
The vacuum interrupter having the above configuration was incorporated in a circuit as a capacitor opening / closing, and the flashover probability was investigated. The test method is 66kV-60
It is set to be equivalent to the switching condition of the MVA capacitor capacity. The conditions for making the DC voltage are 54kVr.ms to the capacitor in advance.
Was charged, and a current of 3700 A peak and 200 cycles was applied by LC vibration. On the other hand, the power supply voltage of 50 cycles is 50kV.
rms, current of 520A was set as the advance current, and turning on and off was repeated many times under this condition. The gap between the poles is 15 mm, the closing speed is 1 m / sec, and the breaking speed is 2 m / sec.
The results are shown in the following table and FIG.

なお、比較のために、電極3の薄板22を形成する電極材
料として、例えばMo粉末およびCr粉末のそれぞれの粒径
を149μm以下(−100メツシユ)等とし、Cu60重量%,M
o30重量%およびCr10重量%よりなる合金を用いた真空
インタラプタについても前記実施例のものと同一の試験
条件で閃絡確率を調べ、その結果を次表および第4図中
に示した。
For comparison, as an electrode material for forming the thin plate 22 of the electrode 3, for example, Mo powder and Cr powder each have a particle size of 149 μm or less (−100 mesh) or the like, and Cu 60 wt%, M
With respect to the vacuum interrupter using an alloy composed of 30 wt% and 10 wt% Cr, the flashover probability was examined under the same test conditions as those of the above-mentioned examples, and the results are shown in the following table and FIG.

上記表は、試験開閉回数が350回の時点で、MoおよびCr
粉末のそれぞれの粒径が149μm以下(−100メツシユ)
のものを用いた場合の閃絡回数を100%として比較した
ものである。また、表中Moの粒径が平均1〜10μmのも
のは、すべてCrの最大粒径の1/2以下であるという条件
を満足しているものである。
The above table shows that when the number of test opening and closing is 350 times, Mo and Cr
Each particle size of the powder is 149μm or less (-100 mesh)
This is a comparison when the number of flashovers is 100%. Further, in the table, Mo particles having an average particle diameter of 1 to 10 μm all satisfy the condition that they are 1/2 or less of the maximum particle diameter of Cr.

一方、第4図は、横軸に試験開閉回数(回)を、縦軸に
閃絡累積発生回数(回)をとつたものである。第4図
中、実線26は前記実施例によるものの閃絡回数の推移を
示し、破線27はMoおよびCr粉末の各粒径を149μm発下
(−100メツシユ)としたものの閃絡回数の推移を示し
ている。
On the other hand, in FIG. 4, the horizontal axis represents the number of test opening / closing operations (times) and the vertical axis represents the cumulative number of flashover occurrences (times). In FIG. 4, the solid line 26 shows the change in the number of flashovers according to the above-mentioned embodiment, and the broken line 27 shows the change in the flashover counts when the particle diameters of Mo and Cr powders were each smaller than 149 μm (-100 mesh). Shows.

前記表および第4図から判るように、Mo粉末の粒径が最
大74μm以下(−200メツシユ)でかつCr粉末の粒径が
最大149μm以下(−100メツシユ)の場合に、閃絡発生
回数が極めて少なく、安定して多頻度の開閉を行うこと
ができ、コンデンサ開閉用として適している。これは、
MoとCrとの拡散結合が十分に行われているためと思われ
る。また、特にMoの粒径が平均1〜10μmでかつ最大粒
径がCrの1/2以下であるものは、良好である。
As can be seen from the above table and FIG. 4, when the Mo powder particle size is 74 μm or less (−200 mesh) at the maximum and the Cr powder particle size is 149 μm or less (−100 mesh) at the maximum, the number of occurrences of flashover occurs. It is suitable for opening and closing capacitors because it can open and close frequently and stably. this is,
This is probably because diffusion bonding between Mo and Cr is sufficiently performed. Further, particularly, those having an average particle size of Mo of 1 to 10 μm and a maximum particle size of 1/2 or less of Cr are good.

さらに、Cuが55〜80重量%,Moが15〜35重量%およびCr
が4〜12重量%の範囲であれば、同様の結果が得られる
ことが実験により判明した。
In addition, Cu is 55-80 wt%, Mo is 15-35 wt% and Cr
It has been experimentally found that similar results can be obtained in the range of 4 to 12% by weight.

H.発明の効果 以上のように本発明の真空インタラプタの電極材料によ
れば、Cu−Mo−Cr合金の成分組成範囲を限定するととも
に、MoおよびCr粉末の粒径を異ならせて特定しているの
で、MoとCrとの拡散結合が十分に行われ、再点弧の発生
確率が極めて低く、安定して多頻度の開閉を行うことが
でき、コンデンサ開閉用の真空インタラプタの電極材料
として最適である。
H. Effect of the Invention As described above, according to the electrode material of the vacuum interrupter of the present invention, the component composition range of the Cu-Mo-Cr alloy is limited, and the particle sizes of Mo and Cr powders are specified differently. Since Mo and Cr are sufficiently diffusion-bonded, the probability of re-ignition is extremely low, stable and frequent switching can be performed, and it is ideal as an electrode material for a vacuum interrupter for switching capacitors. Is.

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

第1図は本発明の真空インタラプタの電極材料を用いた
電極の縦断正面図、第2図は第1図の部分分解斜視図、
第3図は第1図に示す電極を備えた真空インタラプタの
縦断正面図、第4図は閃絡累積発生回数を示すグラフで
ある。 3…電極、22…薄板、23…接触部、24…アーク拡散部、
25…背面部。
FIG. 1 is a vertical sectional front view of an electrode using an electrode material of a vacuum interrupter of the present invention, and FIG. 2 is a partially exploded perspective view of FIG.
FIG. 3 is a vertical sectional front view of a vacuum interrupter provided with the electrodes shown in FIG. 1, and FIG. 4 is a graph showing the number of cumulative flashover occurrences. 3 ... Electrode, 22 ... Thin plate, 23 ... Contact part, 24 ... Arc diffusion part,
25 ... Rear part.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】モリブデン粉末とクロム粉末とからなる多
孔質基材の空隙を銅で満たしてなる真空インタラプタの
電極材料において、銅55〜80重量%,モリブデン15〜35
重量%およびクロム4〜12重量%の合金からなり、合金
製造前におけるクロムの粒径が149μm以下、モリブデ
ンの最大粒径がクロムの最大粒径の1/2以下としたこと
を特徴とする真空インタラプタの電極材料。
1. A vacuum interrupter electrode material comprising a porous substrate composed of molybdenum powder and chromium powder filled with voids with copper.
% Vacuum and 4-12% by weight of chromium, vacuum characterized in that the grain size of chromium before manufacturing the alloy was 149 μm or less and the maximum grain size of molybdenum was 1/2 or less of the maximum grain size of chromium. Electrode material for interrupter.
【請求項2】合金製造前におけるモリブデンの平均粒径
が1〜10μmであることを特徴とする特許請求の範囲第
1項記載の真空インタラプタの電極材料。
2. The electrode material for a vacuum interrupter according to claim 1, wherein the average particle size of molybdenum before the alloy is manufactured is 1 to 10 μm.
JP6016186A 1986-03-18 1986-03-18 Vacuum interrupter electrode material Expired - Lifetime JPH0693340B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6016186A JPH0693340B2 (en) 1986-03-18 1986-03-18 Vacuum interrupter electrode material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6016186A JPH0693340B2 (en) 1986-03-18 1986-03-18 Vacuum interrupter electrode material

Publications (2)

Publication Number Publication Date
JPS62217519A JPS62217519A (en) 1987-09-25
JPH0693340B2 true JPH0693340B2 (en) 1994-11-16

Family

ID=13134151

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6016186A Expired - Lifetime JPH0693340B2 (en) 1986-03-18 1986-03-18 Vacuum interrupter electrode material

Country Status (1)

Country Link
JP (1) JPH0693340B2 (en)

Also Published As

Publication number Publication date
JPS62217519A (en) 1987-09-25

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