JPH043614B2 - - Google Patents
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- Publication number
- JPH043614B2 JPH043614B2 JP10488185A JP10488185A JPH043614B2 JP H043614 B2 JPH043614 B2 JP H043614B2 JP 10488185 A JP10488185 A JP 10488185A JP 10488185 A JP10488185 A JP 10488185A JP H043614 B2 JPH043614 B2 JP H043614B2
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- Prior art keywords
- vacuum
- degree
- voltage
- waveform
- decrease
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- 230000007423 decrease Effects 0.000 claims description 34
- 239000002184 metal Substances 0.000 claims description 3
- 238000001514 detection method Methods 0.000 description 36
- 238000010586 diagram Methods 0.000 description 9
- 230000010363 phase shift Effects 0.000 description 7
- 230000003247 decreasing effect Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 4
- 239000003990 capacitor Substances 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
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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真空度低下検出
装置に係り、特に系統電位部材と中間シールドの
間のインピーダンス変化を利用して真空度低下を
検出する装置に関する。DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a vacuum level drop detection device for a vacuum interrupter, and in particular detects a vacuum level drop using an impedance change between a grid potential member and an intermediate shield. Regarding equipment.
B 発明の概要
本発明は、系統電位部材と中間シールドの間の
インピーダンス変化を利用して真空度低下を検出
する真空インタラプタの真空度低下検出装置にお
いて、
系統電位部材の電圧波形に対する中間シールド
の電圧波形の変化によつて真空度低下を判定し、
この判定信号を記憶保持しておく構成により、
真空度低下がしや断不能になる圧力まで進行す
る前に検出し、しかも急速な真空度低下にも確実
に検出できるようにしたものである。B. Summary of the Invention The present invention provides a vacuum level drop detection device for a vacuum interrupter that detects a vacuum level drop using an impedance change between a grid potential member and an intermediate shield. Determine the decrease in vacuum level based on changes in the waveform,
By storing this judgment signal in memory, it is possible to detect the decrease in the degree of vacuum before it reaches a pressure that cannot be cut off, and also to be able to reliably detect even a rapid decrease in the degree of vacuum.
C 従来の技術
本来、真空インタラプタは、他の開閉器具に比
べ電気的にも機械的にも長寿命であり、保守点検
を殆んど不要とする。しかし、しや断回数の増大
等に伴う経時的な真空度低下のほかに、非常に稀
ではあるがベローズや気密接合部等からの真空漏
れによつて真空度が急速に低下することがある。
真空インタラプタ(電流しや断部)は、その真空
度低下によりしや断性能が低下し、ひいてはしや
断不能に至る。したがつて、真空インタラプタは
その真空度を定期的に又は常時点検することが要
求されている。C. Prior Art Vacuum interrupters inherently have a longer life both electrically and mechanically than other switching devices, and require almost no maintenance or inspection. However, in addition to the degree of vacuum decreasing over time due to an increase in the number of times the sheath is broken, the degree of vacuum may decrease rapidly due to vacuum leakage from bellows, airtight joints, etc., although this is very rare. .
The vacuum interrupter (current interrupter) has reduced interrupting performance due to a decrease in its degree of vacuum, and eventually becomes unable to interrupt the interrupter. Therefore, the vacuum interrupter is required to periodically or constantly check its vacuum degree.
しかも、真空インタラプタは、操作機構と組立
てられて真空しや断器を構成した後、充電状態で
真空度を正確かつ簡便に検査し得ることが望まれ
ている。 Moreover, it is desired that the vacuum interrupter can accurately and easily test the degree of vacuum in a charged state after being assembled with an operating mechanism to form a vacuum interrupter.
ところで、真空インタラプタの真空度と真空ギ
ヤツプの放電開始電圧とは、第2図に示すよう
に、パツシエンの法則に近似した関係にある。第
2図は、横軸に真空インタラプタ内部圧力、縦軸
に放電開始電圧をとつたもので、図中実線(一部
破線)は真空ギヤツプが10mmの場合の特性を示
す。第2図から判るように、真空インタラプタ内
の真空度が10-4mmHg(13.33mPa)以下の高真空
であれば放電開始電圧は非常に高い。しかし、真
空度が劣化して10-1mmHg(13.33Pa)程度になる
と500Vまで低下する。 By the way, the degree of vacuum of the vacuum interrupter and the discharge starting voltage of the vacuum gap have a relationship similar to Patsien's law, as shown in FIG. In Figure 2, the horizontal axis shows the internal pressure of the vacuum interrupter, and the vertical axis shows the discharge starting voltage.The solid line (partly broken line) in the figure shows the characteristics when the vacuum gap is 10 mm. As can be seen from Figure 2, if the degree of vacuum inside the vacuum interrupter is a high vacuum of 10 -4 mmHg (13.33mPa) or less, the discharge starting voltage is extremely high. However, when the degree of vacuum deteriorates to around 10 -1 mmHg (13.33Pa), the voltage drops to 500V.
従来、このような法則を利用して、しかも充電
状態での真空度監視を行うべく、真空インタラプ
タの開極状態の電極間又は閉極状態において電極
等の系統電位部材と中間シールドとの間の対地電
圧変化から真空度低下を検出するものがある。 Conventionally, in order to monitor the degree of vacuum in the charging state by utilizing such a law, the voltage between the open electrodes of the vacuum interrupter or between the grid potential members such as electrodes and the intermediate shield in the closed state has been proposed. There are devices that detect a decrease in the degree of vacuum from changes in ground voltage.
第3図には開極時の負荷側電極の電圧変化から
検出する場合を示す。真空インタラプタ1は固定
電極2が系統線路側とされ、可動電極3が負荷側
とされる。この真空インタラプタ1の真空度低下
検出装置として、可動電極3の対地電圧E2レベ
ルを検出するインピーダンス素子の直列回路にな
る電圧検出器4と、電極2と3の開極状態で検出
器4の検出レベルが系統線路電圧(固定電極2の
電圧)E1に相当するレベルまで上昇したか否か
によつて真空度低下有無を判別する判別回路5と
が設けられる。 FIG. 3 shows a case where detection is performed from the voltage change of the load side electrode when the contact is opened. The vacuum interrupter 1 has a fixed electrode 2 on the grid line side and a movable electrode 3 on the load side. The vacuum level drop detection device for this vacuum interrupter 1 includes a voltage detector 4 which is a series circuit of impedance elements that detects the ground voltage E2 level of the movable electrode 3, and A determination circuit 5 is provided which determines whether the degree of vacuum has decreased depending on whether the detection level has increased to a level corresponding to the system line voltage (voltage of the fixed electrode 2) E1 .
このうような構成において、真空インタラプタ
1の真空度低下につれて電極2,3間の放電開始
電圧が低下し、ついには電極2,3間に閃絡が発
生する。即ち、真空度低下によつて電極2,3間
で放電が生じ、電極3の電圧E2が上昇し、つい
には電極2の電圧E1にほぼ等しくなり、該電圧
E2の上昇検出によつて真空度低下を検出する。 In such a configuration, as the degree of vacuum in the vacuum interrupter 1 decreases, the discharge starting voltage between the electrodes 2 and 3 decreases, and eventually a flashover occurs between the electrodes 2 and 3. That is, as the degree of vacuum decreases, a discharge occurs between electrodes 2 and 3, and the voltage E 2 of electrode 3 increases until it becomes almost equal to the voltage E 1 of electrode 2, and the voltage
A decrease in the degree of vacuum is detected by detecting a rise in E2 .
第4図には中間シールドの対地電圧変化から検
出する場合を示す。同図においては、中間シール
ド(金属製)6の対地電圧E3を電圧検出器7で
検出し、この検出レベルの変化によつて判定回路
5に真空度低下の有無判定出力を得る。 FIG. 4 shows a case where detection is performed from a change in the ground voltage of the intermediate shield. In the figure, the ground voltage E 3 of the intermediate shield (made of metal) 6 is detected by the voltage detector 7, and based on the change in this detection level, an output for determining whether or not the degree of vacuum has decreased is obtained from the determination circuit 5.
この検出装置では、第3図のものに比べて電極
2,3の開極状態、閉極状態に拘らず電極2が充
電されている限り、真空度低下を検出可能とす
る。 Compared to the one shown in FIG. 3, this detection device can detect a decrease in the degree of vacuum as long as the electrode 2 is charged regardless of whether the electrodes 2 and 3 are in an open or closed state.
D 発明が解決しようとする問題点
従来の真空度低下検出装置は、電極3の電圧
E2又は中間シールド6の電圧E3を検出するもの
で、いずれも対地電圧の絶対値変化から真空度低
下の判定を得ている。このため、系統電位の変動
や重畳高周波ノイズの影響を受けやすくなり、真
空インタラプタがしや断能力を有する真空度低下
初期での検出ができない問題があつた。D Problems to be solved by the invention The conventional vacuum level drop detection device
It detects the voltage E 2 or the voltage E 3 of the intermediate shield 6, and in both cases, a decrease in the degree of vacuum is determined from the change in the absolute value of the ground voltage. For this reason, it becomes susceptible to fluctuations in the system potential and superimposed high-frequency noise, and there is a problem in that it is not possible to detect the early stage of a decrease in the degree of vacuum, which the vacuum interrupter has the ability to interrupt.
即ち、真空度低下検出感度を高くすると系統電
位変動やノイズによつて誤つた検出をすることに
なるし、逆に検出感度を低くすると電極2,3間
又は電極2と中間シールド間が閃絡状態になるま
で検出できないため、そのとき真空インタラプタ
は既にしや断不能状態にある。 In other words, if the vacuum level drop detection sensitivity is increased, erroneous detection will occur due to system potential fluctuations and noise, and conversely, if the detection sensitivity is decreased, there will be a flash short between electrodes 2 and 3 or between electrode 2 and the intermediate shield. Since it cannot be detected until the vacuum interrupter is in the uninterrupted state, the vacuum interrupter is already in the uninterruptible state.
また、従来の検出装置では、例えばベローズに
発生したピンホール等による真空漏れによつて真
空度が急速に低下し、大気圧近くまで圧力上昇が
あると、真空度低下の検出失敗になる問題があつ
た。即ち、大気圧近くまでの真空度低下が発生す
ると、前記第2図のパツシエンの特性にも示され
るように、大気圧P点では該特性に従つて一度低
下した放電開始電圧が回復して耐電圧特性はある
程度良好となつているために、例えば当該真空イ
ンタラプタの使用電圧が第2図における系統電位
Vよりも低ければ、検出装置の判定出力は真空度
良好という誤つた判定になる。 In addition, with conventional detection devices, if the degree of vacuum rapidly decreases due to vacuum leakage due to a pinhole, etc. in the bellows, and the pressure rises to near atmospheric pressure, there is a problem that detection of a decrease in the degree of vacuum may fail. It was hot. In other words, when the degree of vacuum decreases to near atmospheric pressure, as shown in the characteristics of the vacuum cleaner shown in Fig. 2, at the atmospheric pressure point P, the discharge starting voltage that once decreased recovers according to the characteristics, and the withstand voltage increases. Since the voltage characteristics are good to some extent, for example, if the operating voltage of the vacuum interrupter is lower than the system potential V in FIG. 2, the judgment output of the detection device will be an erroneous judgment that the degree of vacuum is good.
E 問題点を解決するための手段
本発明は上記問題点に鑑みてなされたもので、
真空インタラプタに接続される系統電位部材の対
地電圧波形を検出する第1の検出器と、中間シー
ルドの対地電圧波形を検出する第2の検出器と、
第1の検出器の検出波形に対する第2の検出器の
検出波形の変化によつて真空インタラプタの真空
度低下の判定信号を得る判定回路と、この判定回
路の判定信号を記憶保持する記憶保持回路とを備
えた真空度低下検出装置とするものである。E Means for Solving the Problems The present invention has been made in view of the above problems.
a first detector that detects a ground voltage waveform of a grid potential member connected to the vacuum interrupter; a second detector that detects a ground voltage waveform of an intermediate shield;
A determination circuit that obtains a determination signal of a decrease in the degree of vacuum of the vacuum interrupter based on a change in the detection waveform of a second detector relative to the detection waveform of the first detector, and a memory holding circuit that stores and retains the determination signal of this determination circuit. This is a vacuum level drop detection device equipped with the following.
F 作用
判定回路の判定出力を記憶保持することによつ
て真空度低下が急速に大気圧まで進行した場合に
も検出出力の消滅を無くす。F Effect By storing the determination output of the determination circuit, the detection output is prevented from disappearing even when the degree of vacuum rapidly decreases to atmospheric pressure.
また、第2の検出器の検出波形の比較基準を系
統電位部材の検出波形とすることによつて系統電
位の変動や重畳高周波ノイズによる影響を無く
す。 Further, by using the detected waveform of the grid potential member as a comparison standard for the detected waveform of the second detector, the effects of fluctuations in the grid potential and superimposed high-frequency noise are eliminated.
また、検出波形の比較による検出、即ち検出信
号の比較に振幅(電圧)に限ることなく位相差、
波形歪みも含めた比較検出によつて真空度低下が
しや断不能まで進行する前に検出できるようにす
る。この点について以下に詳細に説明する。 In addition, detection by comparing detection waveforms, that is, comparison of detection signals is not limited to amplitude (voltage), but also phase difference,
By comparative detection including waveform distortion, it is possible to detect a decrease in the degree of vacuum before it progresses to the point where it cannot be cut off. This point will be explained in detail below.
本発明者等は、真空インタラプタにおける真空
度と中間シールドの電圧波形の相関性について研
究した結果、真空度低下初期にあつても検出波形
に位相変化及び波形歪み量変化を現れることを実
験結果から得ることができたし、等価回路からの
演算結果としても得ることができた。 As a result of researching the correlation between the degree of vacuum and the voltage waveform of the intermediate shield in a vacuum interrupter, the inventors of the present invention found from experimental results that even in the early stages of decreasing the degree of vacuum, a phase change and a change in the amount of waveform distortion appear in the detected waveform. I was able to obtain it, and I was also able to obtain it as a calculation result from the equivalent circuit.
この実験例として、前述の第4図における中間
シールド6の検出電圧波形e3と、電極2の検出電
圧波形e1を観測し、これら波形e3,e1には第5図
及び第6図に示すものを得た。第5図は真空度低
下初期(第2図に示す真空度P1)に局部的に放
電が生じているときの波形e1,e3を示す。この場
合中間シールド電圧波形e3は波形e1に対して振幅
の変化を少く、波形歪み及び位相ずれを発生して
いる。 As an example of this experiment, the detected voltage waveform e 3 of the intermediate shield 6 and the detected voltage waveform e 1 of the electrode 2 in FIG. 4 mentioned above were observed. I got what is shown below. FIG. 5 shows waveforms e 1 and e 3 when a local discharge occurs at the beginning of a decrease in the degree of vacuum (degree of vacuum P 1 shown in FIG. 2). In this case, the intermediate shield voltage waveform e 3 has a smaller change in amplitude than the waveform e 1 , causing waveform distortion and phase shift.
第6図は真空度がさらに低下(第2図に示す真
空度P2)したときの波形e1,e3を示す。このとき
は各真空ギヤツプにおいて放電、閃絡が生じ、波
形e1に対する波形e3は波形歪みと位相ずれ(遅
れ)の増大に加えて波高値が上昇し、波形e3が波
形e1に近い振幅になる。 FIG. 6 shows waveforms e 1 and e 3 when the degree of vacuum is further reduced (degree of vacuum P 2 shown in FIG. 2). At this time, discharge and flashover occur in each vacuum gap, and waveform e3 with respect to waveform e1 has waveform distortion and phase shift (delay), and the peak value increases, causing waveform e3 to become close to waveform e1. becomes the amplitude.
こうした波形の変化を真空度変化との関係につ
いて、電極2と中間シールド6間のインピーダン
スの変化に基づくものであると見做せることは、
第7図に示す等価回路からのコンピユータ演算に
よつても確認された。第7図において、電極2の
電圧E1をインピーダンス素子Z1,Z2の分圧によ
つて電圧e1として検出し、電極2と中間シールド
6の間のインピーダンスを容量C3と放電抵抗R
の並列になる等価回路とし、中間シールド6の電
圧E3をコンデンサC2,C1の分圧によつて電圧e3
として検出し、真空度低下を放電抵抗Rの低下に
なるとするとき、電圧e1に対する電圧e3の位相ず
れはC3=100pFでは第8図に示す演算結果を得
た。また、同図には抵抗Rの変化による対値電圧
e3(中間シールドの電圧)のレベル変化を合せて
示す。以上までの実験例及び等価回路からの演算
結果から、検出波形の変化、特に位相ずれ又は波
形歪みの変化を監視することによつて真空度低下
をその初期(真空インタラプタがしや断能力を持
つ真空度)に検出できることが判つた。 Regarding the relationship between these changes in waveform and the change in the degree of vacuum, the fact that it can be considered to be based on the change in impedance between the electrode 2 and the intermediate shield 6 is as follows.
This was also confirmed by computer calculations from the equivalent circuit shown in FIG. In FIG. 7, voltage E 1 of electrode 2 is detected as voltage e 1 by voltage division of impedance elements Z 1 and Z 2 , and impedance between electrode 2 and intermediate shield 6 is determined by capacitance C 3 and discharge resistance R.
The voltage E 3 of the intermediate shield 6 is divided into the voltage e 3 by the capacitors C 2 and C 1 .
When the decrease in the degree of vacuum is assumed to be a decrease in the discharge resistance R, the phase shift of the voltage e 3 with respect to the voltage e 1 is C 3 =100 pF, and the calculation results shown in FIG. 8 are obtained. In addition, the figure also shows the relative voltage due to the change in resistance R.
It also shows the level change of e 3 (intermediate shield voltage). From the above experimental examples and the calculation results from the equivalent circuit, it is possible to detect a decrease in the degree of vacuum at its initial stage (when the vacuum interrupter has the ability to It was found that the detection can be performed at a certain degree (degree of vacuum).
G 実施例
第1図は本発明の一実施例を示す回路図であ
る。1は金属製の中間シールド6を固定電極2及
び可動電極3とは絶縁して備える真空インタラプ
タである。この真空インタラプタ1の真空度低下
検出装置として、系統線路に接続される固定電極
2の対地電圧波形を分圧検出するインピーダンス
要素Z1,Z2の直列回路からなる第1の検出器8
と、中間シールド6の対地電圧波形を分圧検出す
るコンデンサC1,C2の直列回路からなる第2の
検出器7と、第1の検出器8の検出波形を比較基
準入力として第2の検出器7の検出波形の位相ず
れの変化が所定角度以上になつたことを検出する
デイジタル式又はアナログ式の位相ずれ判定回路
9と、この判定回路9の判定出力を記憶する記憶
回路10と、この記憶回路9の記憶動作と同時に
真空度低下の警報を発生する警報器11とが設け
られる。G. Embodiment FIG. 1 is a circuit diagram showing an embodiment of the present invention. Reference numeral 1 denotes a vacuum interrupter that includes a metal intermediate shield 6 insulated from the fixed electrode 2 and the movable electrode 3. As a vacuum level drop detection device for this vacuum interrupter 1, a first detector 8 is composed of a series circuit of impedance elements Z 1 and Z 2 that detects a partial voltage waveform of the ground voltage of the fixed electrode 2 connected to the system line.
and a second detector 7 consisting of a series circuit of capacitors C 1 and C 2 that detects the divided voltage waveform of the ground voltage of the intermediate shield 6, and a second detector 7 with the detected waveform of the first detector 8 as a comparison reference input a digital or analog phase shift determination circuit 9 that detects that the change in phase shift of the detected waveform of the detector 7 has exceeded a predetermined angle; and a storage circuit 10 that stores the determination output of the determination circuit 9. Simultaneously with the storage operation of the storage circuit 9, an alarm device 11 is provided which generates an alarm for a decrease in the degree of vacuum.
こうした構成のおいて、電極2と3の開極状
態、閉極状態に拘らず、電極2が充電状態にある
限り、中間シールド6には対地電圧が現われ、検
出器8の検出波形と共に検出器7に検出波形が現
られる。これら両検出器8,7の検出波形は系統
線路電圧波形に相似し、線路電圧の変動、重畳高
周波ノイズの発生には両検出波形が同率で変化す
る。従つて、判定回路9による検出波形変化から
の真空度低下判定に電圧e1を基準とすることで電
圧変動、ノイズによる影響を取除いた検出を行
う。 In such a configuration, as long as electrode 2 is in a charged state, a ground voltage appears on intermediate shield 6, regardless of whether electrodes 2 and 3 are in an open or closed state. A detected waveform appears at 7. The detection waveforms of these two detectors 8 and 7 are similar to the system line voltage waveform, and both detection waveforms change at the same rate when the line voltage fluctuates and superimposed high frequency noise occurs. Therefore, by using the voltage e1 as a reference for determining the degree of vacuum reduction based on the change in the detected waveform by the determination circuit 9, detection is performed in which the effects of voltage fluctuations and noise are removed.
そして、判定回路9は検出電圧e1,e3間の位相
ずれの変化量から判定することで、真空度低下が
しや断不能にまで進行する前(第2図の真空度
P1程度)に検出する。さらに、記憶保持回路1
0によつて判定回路9からの判定出力を記憶保持
することによつて真空インタラプタの真空度が急
速に低下して大気圧に達する場合にも真空度低下
の判定信号を維持し、警報器11の警報動作を継
続させる。 Then, the determination circuit 9 determines from the amount of change in the phase shift between the detected voltages e 1 and e 3 whether the vacuum level has already started to decrease before it can no longer be cut off (as shown in Figure 2).
Detected at around P 1 ). Furthermore, memory holding circuit 1
By storing the judgment output from the judgment circuit 9 using 0, even when the vacuum level of the vacuum interrupter rapidly decreases and reaches atmospheric pressure, the judgment signal of the decrease in the vacuum level is maintained, and the alarm 11 Continue the alarm operation.
なお、実施例においては、真空度低下の判定を
位相ずれの変化から得る場合を示すが、これは波
形歪みの変化から又は両者の組合せからさらには
振幅の変化とを組合せて判定する構成にして一層
確実な判定を得ることができるのは勿論である。 In addition, in the embodiment, a case is shown in which the determination of the degree of vacuum is determined from a change in phase shift, but this may be determined from a change in waveform distortion or a combination of both, or even a change in amplitude. Of course, a more reliable judgment can be obtained.
また、実施例において、真空インタラプタ1の
構造として、中間シールドと系統電位部材との間
に真空度低下時であつてかつしや断可能な真空度
領域で放電する真空ギヤツプを備えることによ
り、検出をより一層確実にすることができる。こ
の理由を以下に詳細に説明する。 In addition, in the embodiment, the structure of the vacuum interrupter 1 is provided with a vacuum gap between the intermediate shield and the grid potential member that discharges in a vacuum range where the vacuum level can be cut off even when the vacuum level is low. can be made even more reliable. The reason for this will be explained in detail below.
本発明者等は、真空インタラプタにおける放電
現象につき検討した結果、第9図に示す特性を得
た。第9図は、横軸に真空インタラプタ内部圧
力、縦軸に放電開始電圧をとつたものである。第
9図中、実線14,実線15及び実線16は、そ
れぞれ真空ギヤツプA,BおよびCの特性を示す
もので、ギヤツプ長はA>B>Cの関係にある。 The present inventors investigated the discharge phenomenon in a vacuum interrupter and obtained the characteristics shown in FIG. 9. FIG. 9 shows the vacuum interrupter internal pressure on the horizontal axis and the discharge starting voltage on the vertical axis. In FIG. 9, solid lines 14, 15, and 16 indicate the characteristics of vacuum gaps A, B, and C, respectively, and the gap lengths have a relationship of A>B>C.
一般に、長ギヤツプは短ギヤツプよりも放電開
始電圧が高いことが知られていたが、このこと
は、第9図から判るように、高真空又は大気圧近
傍での現象であり、10-2mmHg(1.333Pa)前後の
領域では、逆に短ギヤツプの方が長ギヤツプより
も放電開始電圧は高くなつている。 In general, it was known that long gaps have a higher discharge starting voltage than short gaps, but as can be seen from Figure 9, this phenomenon occurs in high vacuum or near atmospheric pressure, and is 10 -2 mmHg. In the region around (1.333 Pa), on the other hand, the discharge start voltage is higher in the short gap than in the long gap.
かかる現象、即ち長ギヤツプと短ギヤツプ間の
放電開始電圧が逆転する現象から、固定電極2と
中間シールド6のと間のギヤツプ長として真空度
低下初期でかつしや断可能な真空度領域で放電す
る長ギヤツプ(例えば第9図の実線14)のもの
とし、固定電極2と可動電極3の開極ギヤツプ及
び可動電極3と中間シールド6のギヤツプを短ギ
ヤツプ(第9図の実線16)とすることにより、
第9図に示すように真空度領域S1又はS2になるし
や断可能領域での中間シールドへの放電を得るこ
とができ、これは真空度低下初期に検出波形の変
化量を大きく得ることになり、検出を一層確実に
する。 Because of this phenomenon, that is, the phenomenon in which the discharge starting voltage between the long gap and the short gap is reversed, the gap length between the fixed electrode 2 and the intermediate shield 6 causes the discharge to occur in the vacuum range where the vacuum level can be cut off at the beginning of the vacuum level drop. The opening gap between the fixed electrode 2 and the movable electrode 3 and the gap between the movable electrode 3 and the intermediate shield 6 are assumed to be short gaps (for example, the solid line 16 in FIG. 9). By this,
As shown in Figure 9, it is possible to obtain a discharge to the intermediate shield in the vacuum region S 1 or S 2 , which can be cut off, and this results in a large change in the detected waveform at the beginning of the vacuum reduction. This makes detection even more reliable.
H 発明の効果
以上のように本発明によれば、線路の対地電圧
波形に対する中間イールドの対地電圧波形の変形
から真空インタラプタの真空度低下を検出し、こ
の検出信号を記憶保持する構成とするため、真空
度低下初期(しや断不能に進行する前)の検出が
できる。しかも検出信号を記憶して急速な真空度
低下にも確実に検出出力、警報を得ることができ
る。さらに、真空度低下初期に放電する真空ギヤ
ツプを備える真空インタラプタとすることによつ
て、真空度低下初期の検出を一層確実にすること
ができる。H. Effects of the Invention As described above, according to the present invention, a decrease in the vacuum degree of the vacuum interrupter is detected from the deformation of the ground voltage waveform of the intermediate yield with respect to the ground voltage waveform of the line, and this detection signal is stored and retained. , it is possible to detect the initial stage of vacuum deterioration (before it progresses to an unstoppable level). Furthermore, by storing the detection signal, it is possible to reliably obtain a detection output and an alarm even when the degree of vacuum drops rapidly. Furthermore, by using the vacuum interrupter with a vacuum gap that discharges at the beginning of a decrease in the degree of vacuum, detection of the beginning of a decrease in the degree of vacuum can be more reliably detected.
第1図は本発明の一実施例を示す回路図、第2
図はパツシエンの法則に基いた特性図、第3図及
び第4図は従来の検出装置回路図、第5図及び第
6図は真空度低下の進行による線路電圧検出波形
に対する中間シールド電圧検出波形の変化を示す
図、第7図は中間シールドのインピーダンス変化
による検出波形の変化を求めるための等価回路
図、第8図は第7図から求めた位相と振幅の特性
図、第9図は真空ギヤツプ長が異なる場合の真空
インタラプタ内部圧力と放電開始電圧との関係を
示す特性図である。
1……真空インタラプタ、2……固定電極、3
……可動電極、6……中間シールド、7……第2
の検出器、8……第1の検出器、9……位相判定
回路、10……記憶保持回路、11……警報器。
Figure 1 is a circuit diagram showing one embodiment of the present invention, Figure 2 is a circuit diagram showing an embodiment of the present invention.
The figure is a characteristic diagram based on Patsien's law, Figures 3 and 4 are circuit diagrams of conventional detection equipment, and Figures 5 and 6 are intermediate shield voltage detection waveforms relative to line voltage detection waveforms due to progress of vacuum reduction. Figure 7 is an equivalent circuit diagram for determining changes in the detected waveform due to changes in impedance of the intermediate shield, Figure 8 is a characteristic diagram of phase and amplitude obtained from Figure 7, and Figure 9 is a diagram showing the change in the detected waveform due to impedance changes in the intermediate shield. FIG. 6 is a characteristic diagram showing the relationship between the internal pressure of the vacuum interrupter and the discharge starting voltage when the gap lengths are different. 1... Vacuum interrupter, 2... Fixed electrode, 3
...Movable electrode, 6...Middle shield, 7...Second
Detector, 8...first detector, 9...phase determination circuit, 10...memory holding circuit, 11...alarm.
Claims (1)
て絶縁して備える真空インタラプタの真空度低下
を検出する装置において、前記真空インタラプタ
に接続される系統電位部材の対地電圧波形を検出
する第1の検出器と、前記中間シールドの対地電
圧波形を検出する第2の検出器と、前記第1の検
出器の検出波形に対する前記第2の検出器の検出
波形の変化量から真空インタラプタの真空度低下
の判定信号を得る判定回路と、この判定回路の判
定信号を記憶保持する記憶保持回路とを備えたこ
とを特徴とする真空インタラプタの真空度低下検
出装置。 2 前記真空インタラプタは中間シールドと系統
電位部材との間に、真空度低下時であつてかつし
や断可能な真空度領域で放電する真空ギヤツプを
備え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真空度低下検出装置。[Scope of Claims] 1. In a device for detecting a decrease in the degree of vacuum of a vacuum interrupter that is provided with a metal intermediate shield insulated from a grid potential member, the ground voltage waveform of a grid potential member connected to the vacuum interrupter is detected. A first detector detects the ground voltage waveform of the intermediate shield, a second detector detects the ground voltage waveform of the intermediate shield, and a vacuum is determined from the amount of change in the detected waveform of the second detector with respect to the detected waveform of the first detector. 1. An apparatus for detecting a decrease in the degree of vacuum of a vacuum interrupter, comprising: a determination circuit that obtains a determination signal of a decrease in the degree of vacuum of the interrupter; and a memory holding circuit that stores and retains the determination signal of the determination circuit. 2. Claim 1, characterized in that the vacuum interrupter is provided with a vacuum gap between the intermediate shield and the grid potential member, which discharges in a vacuum range where the vacuum level can be cut off when the vacuum level is lowered. A device for detecting a decrease in the degree of vacuum of a vacuum interrupter as described in 2.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10488185A JPS61263015A (en) | 1985-05-16 | 1985-05-16 | Vacuum drop detector for vacuum interrupter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10488185A JPS61263015A (en) | 1985-05-16 | 1985-05-16 | Vacuum drop detector for vacuum interrupter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61263015A JPS61263015A (en) | 1986-11-21 |
| JPH043614B2 true JPH043614B2 (en) | 1992-01-23 |
Family
ID=14392528
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10488185A Granted JPS61263015A (en) | 1985-05-16 | 1985-05-16 | Vacuum drop detector for vacuum interrupter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61263015A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01122530A (en) * | 1987-11-06 | 1989-05-15 | Mitsubishi Electric Corp | Breaking performance deterioration predicting device for vacuum breaker |
| JP4686555B2 (en) * | 2008-01-09 | 2011-05-25 | 株式会社日立製作所 | Vacuum switchgear |
| JP6119985B2 (en) * | 2013-07-05 | 2017-04-26 | 日新電機株式会社 | Vacuum valve vacuum degree monitoring method and vacuum valve vacuum degree monitoring apparatus |
| JP6397700B2 (en) * | 2014-09-01 | 2018-09-26 | 株式会社日立産機システム | Vacuum valve pressure diagnostic device or vacuum valve device |
-
1985
- 1985-05-16 JP JP10488185A patent/JPS61263015A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61263015A (en) | 1986-11-21 |
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