JPH0779015B2 - Vacuum interrupter formation method - Google Patents

Vacuum interrupter formation method

Info

Publication number
JPH0779015B2
JPH0779015B2 JP22199587A JP22199587A JPH0779015B2 JP H0779015 B2 JPH0779015 B2 JP H0779015B2 JP 22199587 A JP22199587 A JP 22199587A JP 22199587 A JP22199587 A JP 22199587A JP H0779015 B2 JPH0779015 B2 JP H0779015B2
Authority
JP
Japan
Prior art keywords
vacuum interrupter
formation
current
arc
electrodes
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 - Fee Related
Application number
JP22199587A
Other languages
Japanese (ja)
Other versions
JPS6465736A (en
Inventor
泰司 野田
佳行 柏木
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
Original Assignee
Meidensha Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Meidensha Corp filed Critical Meidensha Corp
Priority to JP22199587A priority Critical patent/JPH0779015B2/en
Publication of JPS6465736A publication Critical patent/JPS6465736A/en
Publication of JPH0779015B2 publication Critical patent/JPH0779015B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01HELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
    • H01H1/00Contacts
    • H01H1/02Contacts characterised by the material thereof
    • H01H1/0203Contacts characterised by the material thereof specially adapted for vacuum switches

Landscapes

  • Arc Welding Control (AREA)
  • High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)

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化成方法に関し、電極の表
面を均一に化成し得るよう工夫したものである。
DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a method for forming a vacuum interrupter, which is devised so that the surface of an electrode can be formed uniformly.

B.発明の概要 本発明は、化成時の真空インタラプタのアークに対し縦
磁界を加えるとともに、化成電流がピークになるとき真
空インタラプタが全開となるように化成電流の周波数を
調整して縦磁界効果が電極表面全体に均一に及び、アー
クが電極表面全体に均一に広がるようにし、電極表面の
均一な化成を行ない得るようにしたものである。
B. Outline of the Invention The present invention applies a longitudinal magnetic field to the arc of the vacuum interrupter during formation, and adjusts the frequency of the formation current so that the vacuum interrupter is fully opened when the formation current peaks. Uniformly spreads over the entire electrode surface, and the arc spreads evenly over the entire electrode surface, so that uniform formation of the electrode surface can be performed.

C.従来の技術 真空遮断器は小形軽量で信頼性も高く、且つ保守も容易
な遮断器として汎用されている。真空遮断器の主要構成
部品は真空インタラプタであり、この真空インタラプタ
では10-5Torr程度の真空容器内に相対向する一対の電極
が導入されており、一方が他方に対して接離することに
より回路を開閉するようになっている。
C. Conventional technology Vacuum circuit breakers are widely used as circuit breakers that are small, lightweight, highly reliable, and easy to maintain. The main component of the vacuum circuit breaker is a vacuum interrupter.In this vacuum interrupter, a pair of electrodes facing each other are introduced in a vacuum container of about 10 -5 Torr, and one of them is brought into contact with and separated from the other. It is designed to open and close circuits.

一方、この真空インタラプタは、高真空状態とすること
が必要であり、その製造工程においてはろう付け時、加
熱排気時において熱負荷を受ける。このため、電極表面
は熱負荷による荒れを起こし、初期において所定の絶縁
耐力及び絶縁回復特性が得られないことがある。そこ
で、この種の真空インタラプタでは、一般に、電極間に
アークを発生させ、このアークにより電極表面の荒れを
洗浄する、所謂電流化成が施されている。
On the other hand, this vacuum interrupter needs to be in a high vacuum state, and in the manufacturing process thereof, it receives a heat load during brazing and during heating and exhausting. For this reason, the electrode surface may be roughened by a heat load, and the predetermined dielectric strength and dielectric recovery characteristics may not be obtained in the initial stage. Therefore, this type of vacuum interrupter is generally subjected to so-called current formation, in which an arc is generated between the electrodes and the arc cleans the surface of the electrodes.

従来技術に係る最も初期の化成方法は、閉極状態の化成
用の真空インタラプタの電極間に交流電圧を印加し、こ
の印加状態を継続したまま電極を開極することにより電
極間にアークを発生させるというものである。
The earliest chemical conversion method according to the related art is to generate an arc between the electrodes by applying an AC voltage between the electrodes of the vacuum interrupter for chemical conversion in the closed state and opening the electrodes while maintaining this applied state. It is to let.

ところが、上記化成方法は、真空インタラプタの電極が
ディスク電極、スパイラル電極及びカップ電極等、縦磁
界型以外の場合、化成により発生するペーパーが真空容
器の内周面に付着してこれを汚損する。このため、化成
回数及び電流値が限定されるので、特に電極の径が大き
くなると充分な化成を行なうことができないという問題
がある。
However, in the above-mentioned chemical conversion method, when the electrodes of the vacuum interrupter are other than the vertical magnetic field type such as the disk electrode, the spiral electrode and the cup electrode, the paper generated by the chemical formation adheres to the inner peripheral surface of the vacuum container and stains it. Therefore, since the number of times of formation and the current value are limited, there is a problem that sufficient formation cannot be performed especially when the diameter of the electrode is large.

かかる問題点を解消し得る化成方法として化成用の真空
インタラプタの外部に配設したコイルにより縦磁界を加
えるという方法が提案されている。
As a chemical conversion method capable of solving such a problem, a method has been proposed in which a longitudinal magnetic field is applied by a coil arranged outside a vacuum interrupter for chemical conversion.

第1図は縦磁界を加える化成方法を実現するための回
路、第4図はそのときの化成電流の波形及び第5図はそ
のときの化成用の真空インタラプタの開極時のストロー
クの波形を夫々示す。
FIG. 1 shows a circuit for realizing a chemical conversion method for applying a longitudinal magnetic field, FIG. 4 shows a waveform of a chemical current at that time, and FIG. 5 shows a waveform of a stroke at the time of opening a vacuum interrupter for chemical conversion at that time. Show each.

第1図中、1は交流電源、2は補助真空遮断器、3は化
成用の真空インタラプタ、4は縦磁界発生用のコイル、
5はコイル4のための交流電源、Dはダイオード、Rは
抵抗、Lはリアクトル、Cはコンデンサである。
In FIG. 1, 1 is an AC power supply, 2 is an auxiliary vacuum circuit breaker, 3 is a vacuum interrupter for chemical formation, 4 is a coil for generating a vertical magnetic field,
5 is an AC power supply for the coil 4, D is a diode, R is a resistor, L is a reactor, and C is a capacitor.

かかる回路を用いて真空インタラプタ3の化成を行う場
合は、コンデンサCに直流電圧を充電し、補助真空遮断
器2及び化成用のインタラプタ3を閉極してL−C回路
により50Hzの振動電流を作り、その後真空インタラプタ
3を開極することによりこの真空インタラプタ3の電極
間にアークを発生させている。このとき、コイル4によ
りアームに対しこのアークと同方向の縦磁界を作用させ
ている。
When the vacuum interrupter 3 is formed by using such a circuit, the capacitor C is charged with a DC voltage, the auxiliary vacuum circuit breaker 2 and the formation interrupter 3 are closed, and an oscillating current of 50 Hz is generated by the LC circuit. After that, the vacuum interrupter 3 is opened to generate an arc between the electrodes of the vacuum interrupter 3. At this time, the coil 4 causes a longitudinal magnetic field in the same direction as this arc to act on the arm.

第5図中、Aは補助真空遮断器2における真空インタラ
プタの閉極位置、Bは真空インタラプタ3の開極開始位
置、Cは真空インタラプタ3の全開位置である。
In FIG. 5, A is the closed position of the vacuum interrupter in the auxiliary vacuum circuit breaker 2, B is the opening start position of the vacuum interrupter 3, and C is the fully open position of the vacuum interrupter 3.

同図と第4図とを併せて参照すれば明らかな通り、真空
インタラプタ3の全開位置Aは化成電流の零点に略一致
している。これは、一般に、真空インタラプタ3を遮断
時の電流が零になった時点でアークを消すように考慮し
て設計してあり、これに合わせて操作器による開極スピ
ードも決定しているからである。
As is clear by referring to FIG. 4 and FIG. 4 together, the fully open position A of the vacuum interrupter 3 substantially coincides with the zero point of the formation current. This is because, in general, the vacuum interrupter 3 is designed in consideration of extinguishing the arc when the current at the time of interruption becomes zero, and the opening speed by the operating device is also determined accordingly. is there.

D.発明が解決しようとする問題点 ところで、縦磁界を加えて電流化成をする場合、上記従
来技術においては、化成電流のピーク時における真空イ
ンタラプタ3の電極間のギャップが短かいため、即ち第
4図に示す化成電流のピーク時には第5図に示すように
電極は全開位置の略半分の位置迄した開極していないた
め、アークが電極表面上で充分拡散しないという問題が
ある。これはコイルを真空インタラプタの外部に配設し
た場合でも、内部に配設した場合でも、即ち縦磁界型の
真空インタラプタの場合でも同様であるが、特に電極の
径が100mm以上と大きくなると電極表面の外周部分が化
成されずに残ってしまうという結果を招来する。
D. Problems to be Solved by the Invention By the way, when current formation is performed by applying a longitudinal magnetic field, in the above-mentioned conventional technique, the gap between the electrodes of the vacuum interrupter 3 at the peak of the formation current is short, that is, At the peak of the formation current shown in FIG. 4, as shown in FIG. 5, the electrode is not opened up to about half the fully opened position, so that there is a problem that the arc does not sufficiently diffuse on the electrode surface. This is the same whether the coil is arranged outside or inside the vacuum interrupter, that is, in the case of a vertical magnetic field type vacuum interrupter, but especially when the diameter of the electrode becomes larger than 100 mm The result is that the outer peripheral portion of the is left unformed and remains.

対策として、1)化成電流の最大値を増やす、2)化成
回数を増やすいう手段が考えられるが、前者は大きな設
備が必要になるばかりでなく電極の中心部が損傷すると
いう問題があり、後者は電極の中心部のみが化成される
だけで効果がないということが判明した。
As a countermeasure, 1) increasing the maximum value of the formation current, 2) increasing the number of formations can be considered, but the former not only requires a large facility but also has the problem that the central part of the electrode is damaged. It was found that only the central part of the electrode was formed, and it had no effect.

本発明は、上記従来技術に鑑み、電極の径が大きくなっ
てもその表面を均一に化成し得る真空インタラプタの化
成方法を提供することを目的とする。
The present invention has been made in view of the above prior art, and an object thereof is to provide a method for forming a vacuum interrupter capable of forming the surface of the electrode uniformly even if the diameter of the electrode is increased.

E.問題点を解決するための手段 上記目的を達成する本発明の構成は、閉極状態の真空イ
ンタラプタの電極間に交流電圧を印加し、この印加状態
を継続したまま電極を開極することにより電極間にアー
クを発生させ、このアークにより電極表面の荒れを洗浄
する真空インタラプタの化成方法において、アークに対
しこのアークと同一方向の磁界をコイルにより加えると
ともに、真空インタラプタの全開時に化成電流の電流値
がピークになるように化成電流の周波数を調整して真空
インタラプタを開極することを特徴とする。
E. Means for Solving the Problems The constitution of the present invention which achieves the above-mentioned object is to apply an AC voltage between the electrodes of the vacuum interrupter in the closed state, and to open the electrodes while maintaining this applied state. An arc is generated between the electrodes by the arc, and in the method of forming a vacuum interrupter that cleans the surface of the electrode by this arc, a magnetic field in the same direction as this arc is applied to the arc by a coil, and the formation current The vacuum interrupter is opened by adjusting the frequency of the formation current so that the current value reaches a peak.

F.作用 上記構成の本発明によれば真空インタラプタが全開とな
ったとき化成電流もピークになる。即ち、電極の全開時
にアークエネルギは最大となり、このためアークは電極
表面の全域に亘って均一に拡散する。
F. Action According to the present invention having the above configuration, the formation current also reaches a peak when the vacuum interrupter is fully opened. That is, the arc energy is maximized when the electrode is fully opened, so that the arc is diffused uniformly over the entire surface of the electrode.

G.実施例 以下本発明を実施例に基づき図面を用いて詳細に説明す
る。
G. Examples Hereinafter, the present invention will be described in detail based on examples with reference to the drawings.

本実施例は第1図に示す回路を用いて真空インタラプタ
3を電流化成するものである。
In this embodiment, the vacuum interrupter 3 is formed into a current by using the circuit shown in FIG.

このときの諸条件は下記の通りである。The various conditions at this time are as follows.

1)化成回路 電圧;4kV、 電流;31.5×▲√▼2kA 2)化成用の真空インタラプタ3 定格電圧;84kV(r.m.s) 定格電流;31.5kA(r.m.s) ギャップ長;60(mm) 電極;直径110(mm)のスパイラル 定格開極スピード;3m/s 上記条件の下で、本実施例では化成電流の電流値がピー
ク時に真空インタラプタの電極が全開となるように化成
電流の周波数を調整する。この周波数の調整はコンデン
サCの容量を一定にしてコイルLのインダクタンスを変
化させることにより容易に達成される。
1) formation circuit voltage: 4kV, current; 31.5 × ▲ √ ▼ 2kA 2) formation vacuum interrupter 3 rated voltage; 84kV (rms) rated current; 31.5kA (rms) gap length; 60 (mm) electrode; diameter 110 (Mm) Spiral Rated opening speed: 3 m / s Under the above conditions, in this embodiment, the frequency of the formation current is adjusted so that the electrode of the vacuum interrupter is fully opened when the current value of the formation current peaks. This frequency adjustment is easily achieved by keeping the capacitance of the capacitor C constant and changing the inductance of the coil L.

第2図の実線は本実施例に係る化成電流の波形を、また
第3図は本実施例に係る真空インタラプタ3の開極時の
ストローク波形を夫夫示す。両図中、Aは補助真空イン
タラプタ2の閉極位置、Bは真空インタラプタ3の開極
開始位置、Cは真空インタラプタ3の全開位置、Dは化
成電流のピーク時である。
The solid line in FIG. 2 shows the waveform of the formation current according to this embodiment, and FIG. 3 shows the stroke waveform when the vacuum interrupter 3 according to this embodiment is opened. In both figures, A is the closing position of the auxiliary vacuum interrupter 2, B is the opening start position of the vacuum interrupter 3, C is the fully open position of the vacuum interrupter 3, and D is the peak of the formation current.

本実施例では真空インタラプタ3の全開位置Cと化成電
流のピーク時Dが一致している。一方、従来技術におけ
る化成電流(50Hz)の波形を第2図中に一点鎖線で示
し、そのピーク時を符号Eで第2図に、またピーク時E
における真空インタラプタ3の開極位置を符号Fで第3
図に夫々示している。第2図に示すように、本実施例の
化成電流は従来技術における化成電流よりも低周波数
(30Hz)としてピーク時Eに対しピークDを遅らしてい
る。
In the present embodiment, the fully open position C of the vacuum interrupter 3 and the peak time D of the formation current match. On the other hand, the waveform of the formation current (50 Hz) in the prior art is shown by the alternate long and short dash line in FIG. 2, and its peak time is indicated by the symbol E in FIG.
The opening position of the vacuum interrupter 3 at
Each is shown in the figure. As shown in FIG. 2, the formation current of this embodiment has a lower frequency (30 Hz) than the formation current in the prior art, and the peak D is delayed with respect to the peak time E.

かかる、本実施例によれば、アークエネルギーが最も大
きい化成電流のピーク時に電極間のギャップが最大とな
るため、縦磁界が電極面全体に作用し、アークを電極面
全体に均一に拡散させる。
According to the present embodiment, since the gap between the electrodes becomes maximum at the peak of the formation current having the highest arc energy, the longitudinal magnetic field acts on the entire electrode surface to uniformly diffuse the arc on the entire electrode surface.

化成条件は前述と同じにし、且つ本発明及び従来におけ
る縦磁界を印加した化成後の真空インタラプタの耐電圧
特性を調べた結果を第6図に示す。
FIG. 6 shows the results of examining the withstand voltage characteristics of the vacuum interrupter after the chemical conversion in the present invention and the conventional one in which the longitudinal magnetic field was applied under the same chemical conversion conditions as described above.

第6図は縦磁界を加えて電流化成を行なった場合のイン
パルス耐電圧特性を示すグラフである。同図中、○印は
本発明による場合、◎印は従来の場合の耐電圧値の平均
をプロットしてある。
FIG. 6 is a graph showing impulse withstand voltage characteristics when current formation is performed by applying a vertical magnetic field. In the figure, the mark ◯ indicates the case of the present invention, and the mark ◎ indicates the average of the withstand voltage values in the conventional case.

第6図から明らかなように、本発明によれば初期より安
定した耐電圧特性が得られることが確認できた。
As is clear from FIG. 6, it was confirmed that according to the present invention, stable withstand voltage characteristics were obtained from the initial stage.

なお、第2図を参照すれば明らかな通り化成電流の周波
数を下げるとそのピーク値も下がるが、真空インタラプ
タ3の全開時にピークとなる周波数の化成電流のピーク
値が所定の電流値になるように電圧値を決定してやれば
問題はない。また、化成電流の周波数は、一般の真空イ
ンタラプタの開極時のストローク波形から考えて40Hz〜
20Hz程度に選定してやれば良い。
As is apparent from FIG. 2, when the frequency of the formation current is lowered, its peak value is also lowered, but the peak value of the formation current at the frequency which becomes a peak when the vacuum interrupter 3 is fully opened becomes a predetermined current value. There is no problem if you decide the voltage value. In addition, the frequency of the formation current is 40Hz, considering the stroke waveform when the general vacuum interrupter opens.
It should be selected to about 20Hz.

更に、前記実施例において縦磁界は外部のコイルにより
発生させたが、これは内部のコイル、即ち縦磁界型の真
空インタラプタのコイルにより発生させても勿論良い。
Further, although the vertical magnetic field is generated by the external coil in the above embodiment, it may be generated by the internal coil, that is, the coil of the vertical magnetic field type vacuum interrupter.

H.発明の効果 以上実施例とともに具体的に説明したように、本発明に
よれば真空インタラプタの全開時に化成電流の電流値が
ピークになるように化成電流の周波数を調整したので、
アークエネルギが最も大きい化成電流のピーク時には電
極間のギャップが最大になっており、したがって縦磁界
が電極面全体に均一に作用する。この結果、電極はその
径が大きくなっても全体的に均一に化成される。
H. Effect of the Invention As specifically described with the above embodiments, according to the present invention, since the frequency of the formation current is adjusted so that the current value of the formation current becomes a peak when the vacuum interrupter is fully opened,
At the peak of the formation current with the highest arc energy, the gap between the electrodes is maximum, so that the longitudinal magnetic field acts uniformly on the entire electrode surface. As a result, the electrode is uniformly formed even if its diameter is increased.

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

第1図は化成用の回路を示す回路図、第2図はその化成
電流の波形を示す波形図、第3図は本実施例に係る化成
用の真空インタラプタの開極時のストローク波形を示す
波形図、第4図は化成電流の波形を示す波形図、第5図
は従来技術に係る化成用の真空インタラプタの開極時の
ストローク波形を示す波形図、第6図は化成時に縦磁界
を加えた本発明と従来における化成後の真空インタラプ
タのインパルス耐電圧特性を示すグラフである。 図面中、 1,5は交流電源,3は真空インタラプタ、4はコイルであ
る。
FIG. 1 is a circuit diagram showing a chemical formation circuit, FIG. 2 is a waveform diagram showing the waveform of the chemical formation current, and FIG. 3 is a stroke waveform when the vacuum interrupter for chemical formation according to this embodiment is opened. Waveform diagram, FIG. 4 is a waveform diagram showing the waveform of the formation current, FIG. 5 is a waveform diagram showing the stroke waveform when the vacuum interrupter for formation according to the prior art is opened, and FIG. 6 is a longitudinal magnetic field during formation. It is a graph which shows the impulse withstand voltage characteristic of the vacuum interrupter after the chemical conversion in this invention added and the conventional. In the drawing, 1 and 5 are AC power supplies, 3 is a vacuum interrupter, and 4 is a coil.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】閉極状態の真空インタラプタの電極間に交
流電圧を印加し、この印加状態を継続したまま電極を開
極することにより電極間にアークを発生させ、このアー
クにより電極表面を洗浄する真空インタラプタの化成方
法において、アークに対しこのアークと同一方向の磁界
をコイルにより加えるとともに、真空インタラプタの全
開時に化成電流の電流値がピークになるように化成電流
の周波数を調整して真空インタラプタを開極することを
特徴とする真空インタラプタの化成方法。
1. An AC voltage is applied between electrodes of a vacuum interrupter in a closed state, and the electrodes are opened while the application state is maintained to generate an arc between the electrodes, and the arc cleans the electrode surface. In the vacuum interrupter formation method described above, a magnetic field in the same direction as the arc is applied to the arc by a coil, and the frequency of the formation current is adjusted so that the current value of the formation current reaches a peak when the vacuum interrupter is fully opened. A method for forming a vacuum interrupter, which comprises opening the electrodes.
JP22199587A 1987-09-07 1987-09-07 Vacuum interrupter formation method Expired - Fee Related JPH0779015B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22199587A JPH0779015B2 (en) 1987-09-07 1987-09-07 Vacuum interrupter formation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22199587A JPH0779015B2 (en) 1987-09-07 1987-09-07 Vacuum interrupter formation method

Publications (2)

Publication Number Publication Date
JPS6465736A JPS6465736A (en) 1989-03-13
JPH0779015B2 true JPH0779015B2 (en) 1995-08-23

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP22199587A Expired - Fee Related JPH0779015B2 (en) 1987-09-07 1987-09-07 Vacuum interrupter formation method

Country Status (1)

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JP (1) JPH0779015B2 (en)

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Publication number Publication date
JPS6465736A (en) 1989-03-13

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