JPH0748341B2 - Vacuum pressure measuring device for vacuum valve for vacuum circuit breaker - Google Patents
Vacuum pressure measuring device for vacuum valve for vacuum circuit breakerInfo
- Publication number
- JPH0748341B2 JPH0748341B2 JP2252306A JP25230690A JPH0748341B2 JP H0748341 B2 JPH0748341 B2 JP H0748341B2 JP 2252306 A JP2252306 A JP 2252306A JP 25230690 A JP25230690 A JP 25230690A JP H0748341 B2 JPH0748341 B2 JP H0748341B2
- Authority
- JP
- Japan
- Prior art keywords
- vacuum
- circuit breaker
- measuring device
- current
- current pulse
- 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.)
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- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
- Measuring Fluid Pressure (AREA)
- Details Of Valves (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は真空遮断器用真空バルブの真空圧力測定装置に
関するものである。The present invention relates to a vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker.
従来の真空バルブの内部真空圧力測定は工場出荷前に真
空バルブ単品で測定しているため、被測定真空圧力容器
を包囲するソレノイドコイルは、励磁磁束密度を大きく
するため巻数を数百巻以上にし、電源容量を余り大きく
しなかつた。あるいは真空圧力測定による真空容器内の
脱ガス効果を抑えるため、電極間に印加する直流高電圧
をサイラトロン等によりパルス印加する方式等がある。
また、実開昭54−30975号公報に示すように、被測定真
空容器を包囲するソレノイドコイルを二重以上にして真
空圧力の測定範囲を拡大したり、公開技報番号第86−50
4号に示すように、電離放射線による先駆放電を利用し
て真空圧力の測定範囲を拡大していた。Since the internal vacuum pressure of conventional vacuum valves is measured with a single vacuum valve before shipment from the factory, the solenoid coil surrounding the vacuum pressure vessel to be measured has several hundred or more turns to increase the excitation magnetic flux density. , The power supply capacity was not increased too much. Alternatively, in order to suppress the degassing effect in the vacuum container due to the vacuum pressure measurement, there is a method in which a direct current high voltage applied between the electrodes is pulsed by a thyratron or the like.
In addition, as disclosed in Japanese Utility Model Publication No. 54-30975, the solenoid coil surrounding the vacuum container to be measured is doubled or more to expand the measurement range of the vacuum pressure, or disclosed in Japanese Patent Laid-Open No. 86-50.
As shown in No. 4, the range of vacuum pressure measurement was expanded by utilizing the precursory discharge by ionizing radiation.
一方、真空遮断器に搭載された真空バルブの真空圧力測
定については、真空バルブの端板にマグネトロン素子を
具備して置く方法が検討されたが、マグネトロン素子が
高価なため、真空遮断器のコストアツプの要因となるの
で実現されていない。また、簡易法では真空遮断器の線
間の容量変化から真空圧力の劣化を検出する方法もある
が、精度も悪く、あまり採用されていない。On the other hand, for measuring the vacuum pressure of the vacuum valve mounted on the vacuum circuit breaker, a method of installing a magnetron element on the end plate of the vacuum valve was considered, but the cost of the vacuum circuit breaker is high because the magnetron element is expensive. It has not been realized because it becomes a factor of. Further, there is a simple method that detects deterioration of the vacuum pressure from the capacitance change between the lines of the vacuum circuit breaker, but the accuracy is poor and it is not often used.
最近の高度に発達した情報化社会において安定した高品
質の電力供給を行うためには、送電,配電の基幹となる
真空遮断器には高信頼性が要求されている。そのために
は真空遮断器のバイタルパーツである真空バルブの使用
寿命予測,すなわち真空圧力推移予測が注目されてい
る。しかしながら前述したように、真空遮断器に搭載し
た状態での測定方法が確立されていない。また、真空バ
ルブ単品の真空圧力測定方式は、被測定容器を包囲する
コイルが大きかつたり、電源設備が大きかつたりするた
め、フイールドで使用している真空遮断器の真空圧力測
定には利用されていない。In order to provide stable and high-quality power supply in the recent highly developed information society, the vacuum circuit breaker, which is the backbone of power transmission and distribution, is required to have high reliability. For that purpose, attention has been paid to the prediction of the service life of the vacuum valve, which is the vital part of the vacuum circuit breaker, that is, the prediction of vacuum pressure changes. However, as described above, the measuring method in the state of being mounted on the vacuum circuit breaker has not been established. In addition, the vacuum pressure measurement method for a single vacuum valve is used for measuring the vacuum pressure of the vacuum circuit breaker used in the field because the coil surrounding the container to be measured is large and the power supply equipment is large. Not not.
現在、一番利用されている方法は、直流高電圧発生器を
用いた直流耐電圧法である。しかし、本方式は内部真空
圧力が3×10-2Torr以上のグロー放電領域の真空度チエ
ツカーとしては有効であるが、真空バルブの保障限界値
である5×10-4Torr以下の値が測定できない。また、真
空バルブの運転中の内部真空圧力は1×10-6Torrから1
×10-4Torrの範囲内にあるため、真空バルブの寿命予測
には、上記範囲内を絶対値で把握する必要がある。Currently, the most used method is a DC withstanding voltage method using a DC high voltage generator. However, this method is effective as a vacuum degree checker in the glow discharge region where the internal vacuum pressure is 3 × 10 -2 Torr or higher, but the value below the guaranteed value of the vacuum valve, 5 × 10 -4 Torr, is measured. Can not. The internal vacuum pressure during operation of the vacuum valve is 1 × 10 -6 Torr to 1
Since it is in the range of × 10 -4 Torr, it is necessary to grasp the above range as an absolute value in order to predict the life of the vacuum valve.
上記従来技術は、真空遮断器に搭載された真空バルブの
内部真空圧力が絶対値で測定できないため、真空バルブ
の寿命予測ができなかつた。In the above prior art, the internal vacuum pressure of the vacuum valve mounted on the vacuum circuit breaker cannot be measured as an absolute value, so that the life of the vacuum valve cannot be predicted.
本発明は以上の点に鑑みなされたものであり、真空遮断
器に搭載された状態の真空バルブの寿命予測および運
搬,取付けを容易にすることを可能とした真空遮断器用
真空バルブの真空圧力測定装置を提供することを目的と
するものである。The present invention has been made in view of the above points, and measures the vacuum pressure of a vacuum valve for a vacuum circuit breaker, which makes it possible to easily predict the life of the vacuum valve mounted in the vacuum circuit breaker, and to facilitate transportation and installation. The purpose is to provide a device.
上記目的は、大電流パルス電流のパルス電流の立上り時
定数を0.1〜5mSに制御することにより、達成される。The above object is achieved by controlling the rising time constant of the pulse current of the large current pulse current to 0.1 to 5 mS.
被測定真空容器(真空バルブ)に搭載された真空バルブ
を包囲し、磁界を励磁するソレノイドコイルは真空バル
ブに装着自在(1〜50巻)に形成した。A vacuum valve mounted on a vacuum container to be measured (vacuum valve) was surrounded, and a solenoid coil for exciting a magnetic field was formed so as to be attachable to the vacuum valve (1 to 50 turns).
大電流パルス電源、制御回路および検出回路を、夫々複
数個に分割自在で、かつ可搬可能に形成した。The high-current pulse power supply, the control circuit, and the detection circuit are formed so as to be divided into a plurality of parts and to be portable.
上記手段を設けたので、イオン電流の発生確率が高くな
つて、真空圧力測定範囲を10-7Torrまで拡大できるよう
になる。Since the above-mentioned means is provided, the probability of generation of ion current is increased, and the vacuum pressure measurement range can be expanded to 10 -7 Torr.
さらに、ソレノイドコイルが真空遮断器に搭載されてい
る真空バルブに装着自在となり、大電流パルス電源、制
御回路および検出回路は夫々複数個に分割自在となる。Further, the solenoid coil can be freely mounted on the vacuum valve mounted on the vacuum circuit breaker, and the large-current pulse power supply, the control circuit, and the detection circuit can be respectively divided into a plurality of parts.
以下、図示した実施例に基づいて本発明を説明する。第
1図から第8図には本発明の一実施例が示されている。
真空遮断器用真空バルブ1の真空圧力測定装置2は、真
空遮断器3に搭載されている真空バルブ1と、この真空
バルブ1中に機密封止された接離自在な電極4,5に高電
圧を印加する直流高圧電源6と、この電源6から電極4,
5に印加される高電圧が所定電圧に達するまでの遅れ時
間を維持する制御回路7と、この制御回路7を介して動
作する大電流パルス電源8と、このパルス電源8の出力
により磁界を発生し、かつ真空バルブ1を包囲して配置
されるソレノイドコイル9とを備えている。そして一対
の電極4,5間を流れるイオン電流の波高値および積分値
を検出回路(イオン電流検出器)10で測定して真空バル
ブ1中の真空圧力を測定する。このように構成された真
空圧力測定装置2で、本実施例では大電流パルス電源8
のパルス電流の立上り時定数を0.1〜5mSに制御した。こ
のようにすることにより、イオン電流の発生確率が高く
なつて、真空圧力測定範囲を10-7Torrまで拡大できるよ
うになり、真空遮断器3に搭載された状態の真空バルブ
1の寿命予測および運搬,取付けを容易にすることを可
能とした真空遮断器用真空バルブ1の真空圧力測定装置
2を得ることができる。Hereinafter, the present invention will be described based on the illustrated embodiments. One embodiment of the present invention is shown in FIGS.
The vacuum pressure measuring device 2 of the vacuum valve 1 for the vacuum circuit breaker has a high voltage applied to the vacuum valve 1 mounted on the vacuum circuit breaker 3 and the detachable electrodes 4 and 5 sealed inside the vacuum valve 1. DC high-voltage power supply 6 for applying
A control circuit 7 that maintains a delay time until the high voltage applied to 5 reaches a predetermined voltage, a high-current pulse power supply 8 that operates via this control circuit 7, and a magnetic field is generated by the output of this pulse power supply 8. And a solenoid coil 9 arranged so as to surround the vacuum valve 1. The peak value and integrated value of the ion current flowing between the pair of electrodes 4 and 5 are measured by the detection circuit (ion current detector) 10 to measure the vacuum pressure in the vacuum valve 1. In the vacuum pressure measuring device 2 configured as described above, the high-current pulse power source 8 is used in this embodiment.
The rise time constant of the pulse current was controlled to 0.1 to 5 mS. By doing so, the probability of generation of the ion current becomes high, and the vacuum pressure measurement range can be expanded to 10 -7 Torr, and the life prediction of the vacuum valve 1 mounted on the vacuum circuit breaker 3 and It is possible to obtain the vacuum pressure measuring device 2 of the vacuum valve 1 for the vacuum circuit breaker, which can be easily transported and attached.
すなわち第1図に示されているように、真空バルブ1は
真空遮断器3に搭載されている。真空遮断器3からの真
空バルブ1の開閉動作指令は絶縁操作ロツド11より伝達
される。真空バルブ1は、絶縁筒12と上下の端板および
ベローズ13により真空気密を保持されている。閉鎖配電
盤との接続は外部端子14,15を介して行う。That is, as shown in FIG. 1, the vacuum valve 1 is mounted on the vacuum circuit breaker 3. An opening / closing operation command of the vacuum valve 1 from the vacuum circuit breaker 3 is transmitted from an insulating operation rod 11. The vacuum valve 1 is kept airtight by an insulating cylinder 12, upper and lower end plates and a bellows 13. Connection to the closed switchboard is made via external terminals 14 and 15.
第1図の状態で真空圧力を測定するためには、ソレノイ
ドコイル9を真空バルブ1に装着する。この時、真空バ
ルブ1が絶縁碍子やモールド製の絶縁カバー(いずれも
図示せず)に固着されているため、ソレノイドコイル9
の装着は容易でない。そのため、絶縁碍子あるいは絶縁
カバーと真空バルブ1との空隙および相間空隙を考慮し
て、ソレノイドコイル9の巻数は50巻から1巻の範囲と
なる。To measure the vacuum pressure in the state shown in FIG. 1, the solenoid coil 9 is attached to the vacuum valve 1. At this time, since the vacuum valve 1 is fixed to an insulator or a molded insulating cover (neither is shown), the solenoid coil 9
Is not easy to install. Therefore, the number of turns of the solenoid coil 9 is in the range of 50 to 1 in consideration of the space between the insulator or the insulating cover and the vacuum valve 1 and the space between the phases.
真空圧力測定装置2は、直流高電圧電源6,大電流パルス
電源8,検出回路10,直流高電圧を接地する接地スイツチ1
6および接地抵抗17,電源6および機器を制御し、かつイ
オン電流を表示する表示器を具備している制御回路7か
ら構成されている。The vacuum pressure measuring device 2 includes a DC high voltage power supply 6, a large current pulse power supply 8, a detection circuit 10, and a ground switch 1 for grounding the DC high voltage.
6 and a grounding resistance 17, a power supply 6 and a control circuit 7 for controlling the equipment and having an indicator for displaying the ion current.
大電流パルス電源8は第2図に示す回路構成になつてい
る。8aは電源、8b,8l,8oは制限抵抗、8c,8m,8pはパルス
発生回路を示す。各パルス発生回路8c,8m,8pは、リアク
タンスと容量とで構成される。パルス発生回路8cはリア
クタンス8e,8g,8jと容量8d,8f,8h,8iで構成されてい
る。他のパルス発生回路8m,8pも基本構成はパルス発生
回路8cと同じである。同図表示のパルス発生回路内の鎖
線は、インダクタンスと容量との組合せを任意に行える
ようにし、後述の励磁電流波形を形成するものである。
また、パルス発生回路8c,8m,8pを鎖線で接続しているの
も、任意に並列接続できることを示すものである。パル
ス発生回路8c,8m,8pの出力側に夫々放電スイツチ8k,8n,
8qを設置し、最終段のパルス発生回路8pにはパルス波形
整形器8rを具備させた。そしてこの大電流パルス電源の
出力端にソレノイドコイル9を接続する。The high-current pulse power supply 8 has a circuit configuration shown in FIG. 8a is a power supply, 8b, 8l, 8o are limiting resistors, and 8c, 8m, 8p are pulse generating circuits. Each pulse generation circuit 8c, 8m, 8p is composed of reactance and capacitance. The pulse generation circuit 8c is composed of reactances 8e, 8g, 8j and capacitors 8d, 8f, 8h, 8i. The other pulse generating circuits 8m and 8p have the same basic configuration as the pulse generating circuit 8c. The chain line in the pulse generating circuit shown in the figure is for allowing an arbitrary combination of inductance and capacitance to form an exciting current waveform described later.
In addition, the fact that the pulse generation circuits 8c, 8m, and 8p are connected by a chain line also shows that they can be arbitrarily connected in parallel. The discharge switches 8k, 8n, 8n,
8q was installed, and the pulse generation circuit 8p at the final stage was equipped with a pulse waveform shaper 8r. Then, the solenoid coil 9 is connected to the output end of this high-current pulse power supply.
この大電流パルス電源の動作を、次に説明する。電源8a
より各制限抵抗8b,8l,8oを経て各パルス発生回路8c,8m,
8pの容量(例えば発生回路8cについては8d,8f,8h,8i)
に充電される。充電が完了した時点で放電スイツチ8k,8
n,8qを時間遅れをもつて導通すると、パルス発生回路8
c,8m,8pを重畳した電流波形を形成することができる。
最終段のパルス波形整形器8rでパルス電流波形の波尾を
成形している。The operation of this high-current pulse power supply will be described below. Power supply 8a
Through each limiting resistor 8b, 8l, 8o, each pulse generator circuit 8c, 8m,
8p capacitance (eg 8d, 8f, 8h, 8i for generator 8c)
Will be charged. Discharging switch 8k, 8 when charging is completed
When n and 8q are turned on with a time delay, the pulse generator circuit 8
A current waveform in which c, 8m, and 8p are superimposed can be formed.
The pulse wave shaper 8r at the final stage shapes the wave tail of the pulse current waveform.
第3図には、真空圧力測定装置の簡単なタイムチヤート
が示されている。大電流パルス電源8(第1図参照)は
既に充電完了の状態であることを前提とする。図中Aは
直流高電圧、Bはパルス励磁電流、Cはイオン電流を示
す。まず、直流高電圧電源6(第1図参照)のスイツチ
がONされると、直流高電圧が所定電圧に達するまでT1の
時間遅れがある。T1になつたらT3後にパルス電源8(第
1図参照)の放電スイツチをONして、パルス電流Bを通
電する。イオン電流Cは若干の時間遅れで発生する。こ
の時、直流高電圧Aは、所定電圧をT2秒持続する。ま
た、パルス電流BについてもT5秒持続させる必要があ
る。FIG. 3 shows a simple time chart of the vacuum pressure measuring device. It is premised that the high-current pulse power source 8 (see FIG. 1) is already in the charging completed state. In the figure, A is a DC high voltage, B is a pulse excitation current, and C is an ion current. First, when the switch of the DC high voltage power supply 6 (see FIG. 1) is turned on, there is a time delay of T 1 until the DC high voltage reaches a predetermined voltage. After reaching T 1 , the discharge switch of the pulse power source 8 (see FIG. 1) is turned on after T 3 , and the pulse current B is supplied. The ionic current C is generated with a slight time delay. At this time, the DC high voltage A maintains the predetermined voltage for T 2 seconds. Also, the pulse current B must be maintained for T 5 seconds.
第4図はパルス電流Bの波形をモデル化した図形であ
る。波高値の63%に達する時定数τは、回路定数とソレ
ノイドコイル9(第1図参照)のリアクタンスとにより
決定される。W1はパルス発生回路8c(第2図参照)のみ
の波形で、W2はパルス発生回路8m,8p(第2図参照)を
重畳した波形である。T4は波高値の50%の電流h50の時
間を示す。FIG. 4 is a diagram in which the waveform of the pulse current B is modeled. The time constant τ that reaches 63% of the peak value is determined by the circuit constant and the reactance of the solenoid coil 9 (see FIG. 1). W 1 is a waveform of only the pulse generating circuit 8c (see FIG. 2), and W 2 is a waveform in which the pulse generating circuits 8m and 8p (see FIG. 2) are superimposed. T 4 shows the time of the current h 50 of 50% of the peak value.
第5図は真空圧力とイオン電流形成時間tとの関係を示
す。イオン電流形成時間とは、真空バルブ1(第1図参
照)の電極間に電圧を印加し、真空バルブ1を包囲した
ソレノイドコイル9(共に第1図参照)のパルス電流を
通電して励磁した瞬間から真空バルブ内のガス分子がイ
オン化し、イオン電流が形成されるまでの時間である。
イオン電流の検出は、イオン電流が形成されなければで
きないので、イオン電流が形成されるまでの時間、パル
ス電流のh50(第4図参照)を持続させる必要がある。
同図の直線aはソレノイドコイル9(第1図参照)の巻
数が数千巻の従来方式によるイオン化時間を示す。直線
bはそのイオン化電流形成時間を示す。直線cはソレノ
イドコイル9(第1図参照)の巻数を50巻以下にし、パ
ルス電流の立ち上り時定数τ(第3図および第4図参
照)を5mS以下にした時のイオン化時間であり、直線d
はその時のイオン化電流形成時間である。真空圧力Pが
10-6Torrの時はh50のT4時間(第4図参照)は10mS必要
であることが示されている。真空圧力測定下限値を拡大
した場合、例えばP=10-8Torrにした時、イオン化電流
形成時間dは1Sとなり、パルス発生回路は数十段とな
り、電源が膨大となる。本発明は、フイールドで使用で
きる装置の提供であるので、真空圧力測定の範囲が10-6
Torr以上であればよいので、T4(第4図参照)は50mS程
度持続すればよい。FIG. 5 shows the relationship between the vacuum pressure and the ion current formation time t. The ion current formation time means the voltage is applied between the electrodes of the vacuum valve 1 (see FIG. 1), and the pulse current of the solenoid coil 9 (both see FIG. 1) surrounding the vacuum valve 1 is passed to be excited. It is the time from the moment when the gas molecules in the vacuum valve are ionized and an ionic current is formed.
Since the ion current cannot be detected unless the ion current is formed, it is necessary to maintain the pulse current h 50 (see FIG. 4) until the ion current is formed.
The straight line a in the same figure shows the ionization time in the conventional method in which the number of turns of the solenoid coil 9 (see FIG. 1) is several thousand. The straight line b shows the ionization current formation time. The straight line c is the ionization time when the number of turns of the solenoid coil 9 (see FIG. 1) is 50 or less and the rising time constant τ (see FIGS. 3 and 4) of the pulse current is 5 mS or less, d
Is the ionization current formation time at that time. Vacuum pressure P is
10 -6 when Torr is h 50 of T 4 hours (see FIG. 4) has been shown to be required 10 mS. When the lower limit of vacuum pressure measurement is expanded, for example, when P = 10 −8 Torr, the ionization current formation time d becomes 1 S, the pulse generation circuit becomes several tens of stages, and the power supply becomes huge. The present invention provides a device that can be used in the field, so that the range of vacuum pressure measurement is 10 -6.
As long as it is equal to or higher than Torr, T 4 (see FIG. 4) should last about 50 mS.
第6図はソレノイドコイル9(第1図参照)が励磁する
磁界のアンペア・ターン(A・T)とイオン電流が検出
できる真空圧力の範囲とを示す。曲線e,f,g,hの右上を
斜線で示しているのは、その部分がイオン電流の検出で
きることを示す。この曲線e,f,g,hはソレノイドコイル
9(第1図参照)を3,30,300,3000巻にし、励磁電流を
通電した時のイオン電流検出の下限界値の包絡線を示
す。しかし、各々のソレノイドコイルに同じ電流を通電
したのではなく、第1表の励磁電流源に示すようにし
た。すなわち3000巻、300巻は直流定電流を通電し、30
巻,3巻については上述の第4図に示すパルス電流を通電
した。第6図は同じ磁界であれば、励磁電流の立上り時
定数が速い程、真空圧力の検出範囲が拡大していること
を示している。第1表は、磁界が30,000A・Tの時のソ
レノイドコイル、励磁電流源、真空圧力の測定下限界、
ヒイールドでの測定の可否を検討したものを示す。同表
に示されているように、ソレノイドコイル3,000巻,300
巻は、真空遮断器に搭載された真空バルブに装着するこ
とは不可能である。30巻,3巻は真空バルブに装着可能で
あるが、パルス電源が大規模になる。従つて真空圧力下
限値と第4図に示すh50のT4秒とを選定し、適切な電源
の大きさを決定することが肝要である。FIG. 6 shows the ampere-turn (AT) of the magnetic field excited by the solenoid coil 9 (see FIG. 1) and the range of vacuum pressure at which the ion current can be detected. The diagonal lines on the upper right of the curves e, f, g, and h indicate that the ion current can be detected at that portion. The curves e, f, g, and h represent the envelope of the lower limit value of the ion current detection when the solenoid coil 9 (see FIG. 1) has 3, 30, 300, and 3000 turns and the exciting current is passed. However, instead of supplying the same current to each solenoid coil, the excitation current source shown in Table 1 was used. That is, 3000 turns and 300 turns carry a constant DC current,
For the windings and 3 windings, the pulse current shown in FIG. 4 was applied. FIG. 6 shows that, in the case of the same magnetic field, the faster the rise time constant of the exciting current, the wider the detection range of the vacuum pressure. Table 1 shows the lower limit of measurement of solenoid coil, exciting current source, vacuum pressure when the magnetic field is 30,000 A · T,
Shown here are the results of examination of the possibility of measurement at the yield. As shown in the table, solenoid coil 3,000 turns, 300
The winding cannot be mounted on a vacuum valve mounted on a vacuum circuit breaker. Volumes 30 and 3 can be attached to a vacuum valve, but the pulse power supply becomes large-scale. Therefore, it is important to select the lower limit of vacuum pressure and the T 4 seconds of h 50 shown in Fig. 4 to determine the appropriate power source size.
すなわち、ソレノイドコイルの巻数を小さくし、大電流
パルス電源のパルス電流の立上り時定数τを0.1〜5mSに
すれば真空圧力測定範囲を 10-7Torrまで広げることができ、真空遮断器に搭載した
状態の真空バルブの真空圧力が測定できるようになるの
である。このようにイオン電流を測定するのに真空圧力
を低い方にし、ソレノイドコイルを小さくして真空遮断
器に搭載されている真空バルブに装着できるようにし、
イオン電流を測定する装置を小型化して、所期の目的を
達成するようにしたのである。That is, if the number of turns of the solenoid coil is reduced and the rise time constant τ of the pulse current of the high current pulse power supply is set to 0.1 to 5 mS, the vacuum pressure measurement range can be increased. It can be expanded to 10 -7 Torr, and the vacuum pressure of the vacuum valve mounted on the vacuum circuit breaker can be measured. In this way, the vacuum pressure is set to the lower side to measure the ion current, and the solenoid coil is made smaller so that it can be attached to the vacuum valve mounted on the vacuum circuit breaker.
The device for measuring the ionic current was downsized to achieve the intended purpose.
しかしながら直流高電圧電源、大電流パルス電源、検出
回路、制御回路を一体にした状態で運搬することはでき
ない。そのため各々を分割して運搬できるようにする必
要がある。直流高電圧電源は単独で運搬できるようにす
るのは容易であるが、大電流パルス電源、制御回路は基
本的には一体構造が望ましい。特に大電流パルス電源
は、通電路が大電流をパルスで通電するため、電磁反撥
力、接続による発熱を抑える対策をする必要がある。However, the DC high voltage power supply, the large current pulse power supply, the detection circuit, and the control circuit cannot be transported together. Therefore, it is necessary to divide each so that they can be transported. Although it is easy to carry the DC high voltage power source independently, it is basically desirable that the high current pulse power source and the control circuit have an integral structure. In particular, in a high-current pulse power supply, a large current is pulsed in the energization path, so it is necessary to take measures to suppress electromagnetic repulsion and heat generation due to connection.
第7図は大電流パルス電源と制御回路とを分割した状態
を示した。最上段に制御回路箱18,2段目に第1段大電流
パルス発生回路箱8c′、3段目に第2段大電流パルス発
生回路箱8m′、最下段に第N段大電流パルス発生回路箱
8p′を配置する。各々の箱18,8c′,8m′,8p′の下には
運搬し易いように車輪19を設ける。2段目以下の箱8
c′,8m′,8p′の上部には車輪袋20を設け、上から箱を
装填した場合に、ガイト兼固定に利用する。また上部前
面にはレバー21を設け、上部後面には連結部保護カバー
(保護蓋)22を設ける。なお同図において31は把手であ
る。次に導体を自動連結するのを第7図および第8図に
より説明する。FIG. 7 shows a state in which the large current pulse power supply and the control circuit are separated. Control circuit box 18 at the top, first stage large current pulse generation circuit box 8c 'at the second stage, second stage large current pulse generation circuit box 8m' at the third stage, and Nth stage large current pulse generation at the bottom Circuit box
Place 8p '. Wheels 19 are provided under each box 18, 8c ', 8m', 8p 'for easy transportation. Box 8 below the second level
A wheel bag 20 is provided on the upper part of c ′, 8m ′, 8p ′, and is used as a guide and fixing when a box is loaded from above. Further, a lever 21 is provided on the front surface of the upper portion, and a connecting portion protective cover (protective lid) 22 is provided on the rear surface of the upper portion. In the figure, 31 is a handle. Next, automatic connection of conductors will be described with reference to FIGS. 7 and 8.
最下段の第N段大電流パルス発生回路箱8p′には複数個
の容量23とリアクタンスとを配置,接続されている。他
の箱8m′と連結するために、導体24を絶縁体25で保持す
る導体24の先端にチユウリツプコンタクト等の連結部26
を配置する。その連結部26の上部には連結部保護カバー
22を設け、カバー復帰バネ27にワイヤ28を接続し、連結
部保護カバー22の一端もワイヤ28に接続する。ワイヤ28
はガイドピン29を介してレバー21に接続するが、レバー
21の一端は蝶番になつている。第2段大電流パルス発生
回路箱8m′も同様の構成になつているが、前方にバー30
が取り付けてあり、このバー30は導体24の下部先端より
長くする。A plurality of capacitors 23 and reactances are arranged and connected to the Nth high-current pulse generator circuit box 8p 'at the bottom. In order to connect to another box 8m ', the connecting portion 26 such as a chuck contact is attached to the tip of the conductor 24 that holds the conductor 24 with the insulator 25.
To place. On the upper part of the connecting part 26, a connecting part protective cover
22 is provided, the wire 28 is connected to the cover return spring 27, and one end of the connecting portion protection cover 22 is also connected to the wire 28. Wire 28
Is connected to lever 21 via guide pin 29,
One end of 21 is hinged. The second-stage high-current pulse generation circuit box 8m 'has a similar structure, but the bar 30
And the bar 30 is longer than the lower tip of the conductor 24.
第N段大電流パルス発生回路箱8p′の上に第2段大電流
パルス発生回路箱8m′を上から装填すると、まず、車輪
19が車輪袋20にガイドされる。車輪19が車輪袋20にガイ
ドされるとバー30がレバー21に当り、ワイヤ28を左側に
引張る際に、ワイヤ28に接続されている連結部保護カバ
ー22が左側にスライドする。連結部保護カバー22も左側
にスライドすると、導体24がさし込まれ連結部26に挿入
され、自動連結する。これと反対に分離する場合は、第
2段大電流パルス発生回路箱8m′を上に持ち上げると、
カバー復帰バネ27により連結部保護カバー22とレバー21
とが元の位置に復帰し、異物や塵埃が連結部26に侵入す
るのを防止できる。When the second stage high current pulse generation circuit box 8m 'is loaded on the Nth stage high current pulse generation circuit box 8p' from above,
19 is guided by the wheel bag 20. When the wheel 19 is guided by the wheel bag 20, the bar 30 hits the lever 21, and when pulling the wire 28 to the left, the connecting portion protection cover 22 connected to the wire 28 slides to the left. When the connecting portion protection cover 22 also slides to the left, the conductor 24 is inserted and inserted into the connecting portion 26, so that automatic connection is established. When separating in the opposite, lift the second stage high current pulse generation circuit box 8m '
With the cover return spring 27, the connection protection cover 22 and the lever 21
It is possible to prevent the foreign matter and dust from entering the connecting portion 26 by returning the and to their original positions.
このように本実施例によれば次に述べるような効果を奏
することができる。As described above, according to this embodiment, the following effects can be obtained.
(1)真空遮断器に搭載された真空バルブにソレノイド
コイルを装置し、真空圧力を絶対値で把握することがで
きる。(1) A vacuum valve mounted on a vacuum circuit breaker can be equipped with a solenoid coil to grasp the vacuum pressure as an absolute value.
(2)従つて、定期的に測定することにより、真空バル
ブの内部真空圧力の寿命予測が可能となり、真空遮断器
の信頼性を向上することができる。(2) Therefore, it is possible to predict the life of the internal vacuum pressure of the vacuum valve by regularly measuring, and it is possible to improve the reliability of the vacuum circuit breaker.
(3)本装置を分割して可搬型にしたので、あらゆるフ
イールドに利用することができる。(3) Since this device is divided and made portable, it can be used for all fields.
上述のように本発明は真空遮断器に搭載された状態の真
空バルブの寿命予測および運搬,取付けが容易となつ
て、真空遮断器に搭載された状態の真空バルブの寿命予
測および運搬,取付けを容易にすることを可能とした真
空遮断器用真空バルブの真空圧力測定装置を得ることが
できる。INDUSTRIAL APPLICABILITY As described above, the present invention facilitates the life prediction, transportation and installation of the vacuum valve mounted on the vacuum circuit breaker, and the life prediction, transportation and mounting of the vacuum valve mounted on the vacuum circuit breaker. It is possible to obtain a vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker that can be easily made.
第1図は本発明の真空遮断器用真空バルブの真空圧力測
定装置の一実施例の回路構成を示す説明図、第2図は同
じく一実施例の大電流パルス電源の回路図、第3図は同
じく一実施例のタイムチヤート図、第4図は同じく一実
施例のパルス電流波形図、第5図は同じく一実施例の真
空圧力とイオン電流形成時間との関係を示す特性図、第
6図は同じく一実施例の磁界強度によるイオン電流検出
可能な真空圧力範囲を示す特性図、第7図は同じく一実
施例の大電流パルス電源と制御回路とを分割した状態を
示す斜視図、第8図は同じく一実施例の分割したパルス
発生回路箱を自動連結する状態を示す縦断側面図であ
る。 1…真空バルブ(被測定真空容器)、2…真空圧力測定
装置、3…真空遮断器、4,5…電極、6…直流高電圧電
源、7…制御回路、8…大電流パルス電源、8c′…第1
段大電流パルス発生回路箱、8m′…第2段大電流パルス
発生回路箱、8p′…第N段大電流パルス発生回路箱、9
…ソレノイドコイル、10…検出回路、22…連結部保護カ
バー(保護蓋)、26…連結部。FIG. 1 is an explanatory view showing a circuit configuration of an embodiment of a vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker of the present invention, FIG. 2 is a circuit diagram of a large current pulse power supply of the same embodiment, and FIG. Similarly, a time chart of one embodiment, FIG. 4 is a pulse current waveform diagram of the same embodiment, and FIG. 5 is a characteristic diagram showing a relationship between vacuum pressure and ion current formation time of the same embodiment, FIG. Is a characteristic diagram showing a vacuum pressure range in which an ion current can be detected by magnetic field strength of one embodiment, and FIG. 7 is a perspective view showing a state in which a large current pulse power supply and a control circuit of one embodiment are divided. The figure is also a vertical side view showing a state in which the divided pulse generating circuit boxes of one embodiment are automatically connected. 1 ... Vacuum valve (measurement vacuum container), 2 ... vacuum pressure measuring device, 3 ... vacuum circuit breaker, 4,5 ... electrode, 6 ... DC high voltage power supply, 7 ... control circuit, 8 ... large current pulse power supply, 8c ′… First
8th stage high current pulse generator circuit box, 8m '... 2nd stage high current pulse generator circuit box, 8p' ... Nth stage high current pulse generator circuit box, 9
… Solenoid coil, 10… Detection circuit, 22… Coupling part protective cover (protective lid), 26… Coupling part.
Claims (7)
器と、この被測定真空容器中に気密封止された接離自在
な電極に高電圧を印加する直流高電圧電源と、この電源
から前記電極に印加される高電圧が所定電圧に達するま
での遅れ時間を維持する制御回路と、この制御回路を介
して動作する大電流パルス電源と、このパルス電源の出
力により磁界を発生し、かつ前記被測定真空容器を包囲
して配置されるソレノイドコイルとを備え、前記一対の
電極間を流れるイオン電流の波高値および積分値を検出
回路で測定して前記被測定真空容器中の真空圧力を測定
する真空遮断器用真空バルブの真空圧力測定装置におい
て、前記大電流パルス電源のパルス電流の立上り時定数
を0.1〜5mSに制御してなることを特徴とする真空遮断器
用真空バルブの真空圧力測定装置。1. A vacuum container to be measured mounted on a vacuum circuit breaker, a DC high-voltage power supply for applying a high voltage to a freely separable electrode hermetically sealed in the vacuum container to be measured, and this power supply. From the control circuit for maintaining a delay time until the high voltage applied to the electrode reaches a predetermined voltage, a high-current pulse power source that operates via this control circuit, and a magnetic field is generated by the output of this pulse power source, And a solenoid coil disposed so as to surround the vacuum container to be measured, and the peak value and integrated value of the ion current flowing between the pair of electrodes are measured by a detection circuit to measure the vacuum pressure in the vacuum container to be measured. In a vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker for measuring, the vacuum time for a vacuum valve for a vacuum circuit breaker, characterized in that the rising time constant of the pulse current of the large current pulse power supply is controlled to 0.1 to 5 mS. Force measuring device.
波高値が1,000Aから10,000Aの出力を有し、立上りから
波高値の50%までの電流通電幅を10から50mS持続する波
形整形機能を有しているものである請求項1記載の真空
遮断器用真空バルブの真空圧力測定装置。2. The high-current pulse power supply has a waveform with a peak value of 1,000 A to 10,000 A for a large-current pulse, and a waveform shaping for maintaining a current-carrying width of 10 to 50 mS from the rise to 50% of the peak value. The vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker according to claim 1, which has a function.
に搭載されている被測定真空容器に装着自在に形成され
たものである請求項1記載の真空遮断器用真空バルブの
真空圧力測定装置。3. The vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker according to claim 1, wherein the solenoid coil is formed so as to be attachable to a vacuum container to be measured mounted on the vacuum circuit breaker.
である請求項1記載の真空遮断器用真空バルブの真空圧
力測定装置。4. The vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker according to claim 1, wherein the solenoid coil has 1 to 50 turns.
出回路が、夫々複数個に分割自在で、かつ可搬可能に形
成されたものである請求項1記載の真空遮断器用真空バ
ルブの真空圧力測定装置。5. The vacuum pressure of a vacuum valve for a vacuum circuit breaker according to claim 1, wherein the high-current pulse power supply, the control circuit, and the detection circuit are formed so as to be divided into a plurality of parts and to be portable. measuring device.
パルス発生回路箱に収納して分割構成され、かつこれら
回路箱の通電路が上位段の回路箱を装填することにより
自動的に連結されるものである請求項1記載の真空遮断
器用真空バルブの真空圧力測定装置。6. The large-current pulse power source is housed in a plurality of large-current pulse generating circuit boxes and is divided into parts, and the energization paths of these circuit boxes are automatically loaded by loading the upper-level circuit boxes. The vacuum pressure measuring device for a vacuum valve for a vacuum circuit breaker according to claim 1, which is connected.
路の連結部への前記通電路の装填に同期して作動する保
護蓋が設けられたものである請求項6記載の真空遮断器
用真空バルブの真空圧力測定装置。7. The vacuum circuit breaker for a vacuum circuit breaker according to claim 6, wherein the high-current pulse generating circuit box is provided with a protective lid that operates in synchronization with loading of the energizing path into the connecting part of the energizing path. Vacuum pressure measuring device for vacuum valves.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2252306A JPH0748341B2 (en) | 1990-09-21 | 1990-09-21 | Vacuum pressure measuring device for vacuum valve for vacuum circuit breaker |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2252306A JPH0748341B2 (en) | 1990-09-21 | 1990-09-21 | Vacuum pressure measuring device for vacuum valve for vacuum circuit breaker |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04132131A JPH04132131A (en) | 1992-05-06 |
| JPH0748341B2 true JPH0748341B2 (en) | 1995-05-24 |
Family
ID=17235418
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2252306A Expired - Fee Related JPH0748341B2 (en) | 1990-09-21 | 1990-09-21 | Vacuum pressure measuring device for vacuum valve for vacuum circuit breaker |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0748341B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9031795B1 (en) | 2011-12-13 | 2015-05-12 | Finley Lee Ledbetter | Electromagnetic test device to predict a usable life of a vacuum interrupter in the field |
| US9759773B2 (en) | 2011-12-13 | 2017-09-12 | Finley Lee Ledbetter | System and method to predict a usable life of a vacuum interrupter in the field |
| CN103557988A (en) * | 2013-11-09 | 2014-02-05 | 宁夏天地经纬电力设备工程有限公司 | Rotary electric field probe |
| AU2016280719B2 (en) * | 2015-06-15 | 2019-08-29 | Vacuum Interrupters, Inc. | System and method to predict a usable life of a vacuum interrupter in the field |
| CN109490934B (en) * | 2018-12-19 | 2022-11-25 | 上海平高天灵开关有限公司 | X-ray detection platform for vacuum arc-extinguishing chamber |
| CN116818182B (en) * | 2023-07-06 | 2024-09-13 | 江苏爱斯凯电气有限公司 | Inspection device is used in production of high-voltage vacuum circuit breaker |
-
1990
- 1990-09-21 JP JP2252306A patent/JPH0748341B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04132131A (en) | 1992-05-06 |
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