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JPH0434247B2 - - Google Patents
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JPH0434247B2 - - Google Patents

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Publication number
JPH0434247B2
JPH0434247B2 JP13748485A JP13748485A JPH0434247B2 JP H0434247 B2 JPH0434247 B2 JP H0434247B2 JP 13748485 A JP13748485 A JP 13748485A JP 13748485 A JP13748485 A JP 13748485A JP H0434247 B2 JPH0434247 B2 JP H0434247B2
Authority
JP
Japan
Prior art keywords
vacuum
degree
voltage
intermediate shield
impedance
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP13748485A
Other languages
Japanese (ja)
Other versions
JPS61294725A (en
Inventor
Katsuaki Senba
Masayuki Kano
Mamoru Sugii
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 Electric Manufacturing Co Ltd
Original Assignee
Meidensha Electric Manufacturing Co Ltd
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 Electric Manufacturing Co Ltd filed Critical Meidensha Electric Manufacturing Co Ltd
Priority to JP13748485A priority Critical patent/JPS61294725A/en
Publication of JPS61294725A publication Critical patent/JPS61294725A/en
Publication of JPH0434247B2 publication Critical patent/JPH0434247B2/ja
Granted 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真空度低下検出
装置に関するものである。
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.

B 発明の概要 本発明は、中間シールドを備えた真空インタラ
プタの真空度低下を検出する装置において、 系統電位部材と中間シールドとの間で、真空度
低下時にしや断不能領域に至る以前で固定側又は
可動側のいずれか一方のみにて放電する真空ギヤ
ツプを設けるとともに、中間シールドの対地電位
検出量を真空インタラプタの開閉状態に応じて補
正した信号と系統線路の対地電位検出量との偏差
に基づいて真空度低下を検出するように構成する
ことによつて、 真空度低下を確実に、しかも真空度がまだ高い
時点(リークの初期)で検出することができ、真
空インタラプタの開閉状態の如何に拘らず真空度
低下を正確に検出することを可能とし、更に通電
中において常時真空度監視を行うことができるよ
うにしたものであつて、真空度低下検出後にあつ
てもしや断できるようにしたものである。
B. Summary of the Invention The present invention provides a device for detecting a decrease in the degree of vacuum in a vacuum interrupter equipped with an intermediate shield. In addition to providing a vacuum gap that discharges only on either the side or the movable side, the difference between the detected amount of ground potential of the intermediate shield and the detected amount of ground potential of the system line is corrected according to the open/closed state of the vacuum interrupter. By configuring the system to detect a decrease in the degree of vacuum based on the system, it is possible to reliably detect a decrease in the degree of vacuum at a time when the degree of vacuum is still high (at the beginning of a leak), and to detect whether the vacuum interrupter is open or closed. It is possible to accurately detect a decrease in the degree of vacuum regardless of the situation, and furthermore, it is possible to constantly monitor the degree of vacuum while the power is on, and it can be turned off even after a decrease in the degree of vacuum is detected. It is something.

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
がほとんど不要である。しかし、しや断回数の増
大に伴う真空度低下に加え、非常に稀ではある
が、ベローズや気密接合部等から真空漏れして真
空度が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真空
しや断器としての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、その真空度を定
期的にまたは常時点検することが要求されてい
る。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、通電状態
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。
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 a decrease in the degree of vacuum due to an increase in the number of shear breaks, the degree of vacuum may also decrease due to vacuum leakage from bellows, airtight joints, etc., although this is very rare. A vacuum interrupter (current interrupter) has a reduced degree of vacuum, resulting in a decrease in interrupter performance as a vacuum interrupter, and eventually becomes unable to interrupt the interrupter. Therefore, it is required to regularly or constantly check the degree of vacuum. Moreover, it is desired that the vacuum interrupter can accurately and easily test the degree of vacuum in the energized state after being assembled with an operating mechanism to form a vacuum interrupter.

一方、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7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7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)mは真空ギヤツプが10mmの場合の特性を示
す。第7図から判るように、真空インタラプタ内
の真空度が10-1mmHg(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(13.33mpa)程度になる
と500Vで閃絡してしまう。
On the other hand, 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 FIG. 7, the horizontal axis shows the internal pressure of the vacuum interrupter, and the vertical axis shows the discharge starting voltage. In the figure, the solid line (partially broken line) m shows the characteristics when the vacuum gap is 10 mm. As can be seen from FIG. 7, if the degree of vacuum in the vacuum interrupter is a high vacuum of 10 -1 mmHg (13.33 mpa) or less, the discharge starting voltage is extremely high. However, if the degree of vacuum deteriorates to around 10 -1 mmHg (13.33 mpa), flashover will occur at 500V.

従来このような法則を利用して、真空インタラ
プタの真空度低下を検出する手段が知られてお
り、その一例を第8図、第9図に示す。
Conventionally, means for detecting a decrease in the degree of vacuum of a vacuum interrupter using such a law is known, and an example thereof is shown in FIGS. 8 and 9.

先ず第8図に示すものは、中間シールドの対地
電位上昇を検出して真空度を判定しようとするも
のである。
First, the system shown in FIG. 8 attempts to determine the degree of vacuum by detecting the rise in ground potential of the intermediate shield.

同図において1は真空インタラプタ、2は中間
シールドであり、この中間シールド2は固定電極
棒4aや可動電極棒4b等の系統電位部材(系統
電路と同電位を有する部材)とは絶縁して設けら
れている。21はインピーダンス、22は検出器
であり、中間シールド2はインピーダンス21及
び検出器22を介して大地に接続されている。3
a,3bは補助シールド、40はベローズ、41
a,41bは金属端板、42a,42bは電極で
ある。また43,44は夫々絶縁筒及び封着金具
であり、金属端板41a,41bと共に真空容器
を構成している。
In the figure, 1 is a vacuum interrupter, and 2 is an intermediate shield. This intermediate shield 2 is provided insulated from grid potential members (members having the same potential as the grid circuit) such as the fixed electrode rod 4a and the movable electrode rod 4b. It is being 21 is an impedance, 22 is a detector, and the intermediate shield 2 is connected to the ground via the impedance 21 and the detector 22. 3
a, 3b are auxiliary shields, 40 is a bellows, 41
A and 41b are metal end plates, and 42a and 42b are electrodes. Further, 43 and 44 are an insulating cylinder and a sealing fitting, respectively, and constitute a vacuum container together with the metal end plates 41a and 41b.

このような構成においては、真空劣化が生じた
場合、中間シールド2と系統電位部材との間の絶
縁は破壊され、中間シールド2の電位はほぼ系統
電位まで上昇し、その結果検出器22に電気信号
が供給され、こうして真空度低下を検出すること
ができる。
In such a configuration, when vacuum deterioration occurs, the insulation between the intermediate shield 2 and the grid potential member is broken, the potential of the intermediate shield 2 rises to almost the grid potential, and as a result, the detector 22 receives electricity. A signal is provided so that a decrease in vacuum can be detected.

ところで、真空インタラプタにあつては開極時
における耐電圧特性の向上を図るため、電界分布
状態が固定側と可動側とでほぼ対称となるように
構成されているのが一般的である。即ち、中間シ
ールド2と補助シールド3a,3b、金属端板4
1a,41b等との間の真空ギヤツプは固定側と
可動側とで同一寸法ギヤツプとなつている。
Incidentally, in order to improve the withstand voltage characteristics when the contact is opened, vacuum interrupters are generally constructed so that the electric field distribution state is approximately symmetrical between the fixed side and the movable side. That is, the intermediate shield 2, the auxiliary shields 3a and 3b, and the metal end plate 4.
1a, 41b, etc., the fixed side and the movable side have the same size gap.

このために、第8図の手段では、固定側と可動
側とは先述したように対称形に構成されているの
で、ほぼ同じ真空度で中間シールド2と固定側及
び可動側の両者との間で夫々放電を生じてしま
う。従つてたとえしや断可能な真空領域で真空度
低下を検知し、操作機構(図示省略)を作動させ
て電極42a,42bを開極しても固定側と可動
側とは中間シールド2を介して閃絡しているの
で、結局電流をしや断することができない。
For this purpose, in the means shown in FIG. 8, the fixed side and the movable side are constructed symmetrically as described above, so that the intermediate shield 2 and both the fixed side and the movable side can be connected at almost the same degree of vacuum. discharge occurs in each case. Therefore, even if a decrease in the degree of vacuum is detected in a vacuum region that can be cut off and the operating mechanism (not shown) is activated to open the electrodes 42a and 42b, the fixed side and the movable side are connected via the intermediate shield 2. In the end, the current cannot be cut off because the current is flashing.

更にこのような問題点に加えて、中間シールド
2のみの電位上昇にもとづく検出であるから、系
統電路の電圧変動等の影響を避けるためには、中
間シールド2の対地電位E3がほぼ系統電圧E1
まで上昇した時点で検出するようにしておかねば
ならない。このため、真空度低下を検出した時点
ではもはや定格負荷電流さえもしや断することが
できないほど真空度は低下しているのが現状であ
つた。
In addition to these problems, since the detection is based on the potential rise of only the intermediate shield 2, in order to avoid the influence of voltage fluctuations in the grid circuit, it is necessary to keep the ground potential E3 of the intermediate shield 2 almost equal to the grid voltage. It must be detected when the temperature rises to E1 . Therefore, at the time when a decrease in the degree of vacuum is detected, the degree of vacuum has already decreased to such an extent that even the rated load current cannot be cut off.

また第9図に示すものは電極42a,42b間
を開き、その状態で電圧を印加すると共に電圧の
比較によつて真空度低下の有無を判定しようとす
るものである。(特公昭50−114号公報参照)。
Further, in the case shown in FIG. 9, the electrodes 42a and 42b are opened, a voltage is applied in this state, and the presence or absence of a decrease in the degree of vacuum is determined by comparing the voltages. (Refer to Special Publication No. 114 of 1973).

即ち同図においてCVは開路状態の真空インタ
ラプタのキヤパシタンス、CA,CBは夫々固定電
極棒4a及び可動電極棒4bの対地キヤパシタン
スである。今真空インタラプタ1が開路の状態
で、これに対地電圧Epを印加したとすると、 a−e間の端子電圧EaはEa=Ep b−e間の端子電圧EbはEb=CV/CV+CBEp となる。即ちEa>Ebである。しかし真空インタ
ラプタ1が真空不良であるとa−b間はアーク放
電となつて導通し、しかもこの場合のアーク電圧
は数10V以下で印加電圧Epに比して十分小さいの
でEa≒Ebとみなせる。従つて真空インタラプタ
開路のときにEa>Ebなら正常であり、Ea≒Eb
ら真空不良であると判定できる。尚実際には安全
性等の点から各端子電圧はコンデンサ分圧器で測
定するようにしている。
That is, in the figure, C V is the capacitance of the vacuum interrupter in the open state, and C A and C B are the ground capacitances of the fixed electrode rod 4a and the movable electrode rod 4b, respectively. Now, if vacuum interrupter 1 is in an open state and a ground voltage E p is applied to it, the terminal voltage E a between a and e is E a = E p The terminal voltage E b between b and e is E b = C V /C V +C B E p . That is, E a > E b . However, if the vacuum interrupter 1 has a vacuum failure, there will be an arc discharge between a and b and conduction will occur, and the arc voltage in this case is less than a few tens of volts, which is sufficiently small compared to the applied voltage E p , so E a ≒ E b It can be considered as Therefore, when the vacuum interrupter is open, if E a > E b , it is normal, and if E a ≈ E b , it can be determined that the vacuum is defective. In practice, each terminal voltage is measured using a capacitor voltage divider for safety reasons.

しかしながらこのような手段では、開極状態で
検出を行つているため通電中の常時真空度監視が
できないという問題点がある。
However, this method has a problem in that it is impossible to constantly monitor the degree of vacuum while electricity is being applied because the detection is performed in an open state.

ところで、第8図と第9図との技術を合せた状
態、すなわち、第8図において中間シールドの電
位のみでなく、系統電位を考慮して、中間シール
ド電位と系統電位との両者に基づき、真空度を判
定することを試みた。
By the way, the state in which the techniques of FIG. 8 and FIG. 9 are combined, that is, in FIG. 8, not only the potential of the intermediate shield but also the grid potential is taken into account, and based on both the intermediate shield potential and the grid potential, An attempt was made to determine the degree of vacuum.

つまり、系統電位を考慮してこれを基準にして
中間シールド電位を検出することによつて、電圧
変動の悪影響をなくそうとするものである。
In other words, by taking the grid potential into consideration and detecting the intermediate shield potential using this as a reference, it is attempted to eliminate the adverse effects of voltage fluctuations.

しかしながらこのようなことによつても、第8
図に示す手段の場合と同様な問題が生じた。即ち
固定側と可動側とが対称形に構成されていること
から、ほぼ同じ真空度で中間シールド2と固定側
及び可動側の両者との間で夫々放電を生じてしま
い、電極42a,42bを開極しても、結局中間
シールド2を介して固定側と可動側との間で閃絡
が起こり電流をしや断することができない。
However, even with this, the 8th
A similar problem arose as in the case of the means shown in the figure. That is, since the fixed side and the movable side are constructed symmetrically, electric discharge occurs between the intermediate shield 2 and both the fixed side and the movable side at approximately the same degree of vacuum, causing the electrodes 42a and 42b to Even if the poles are opened, a flashover occurs between the fixed side and the movable side via the intermediate shield 2, and the current cannot be cut off.

D 発明が解決しようとする問題点 以上のように従来技術では真空度低下に伴い
ほぼ同じ真空度で中間シールドと固定側及び可動
側の両者との間で夫々閃絡してしまうことから真
空度低下を検出しても負荷電流をしや断できな
い、電圧変動等の影響を避けるためには検出電
圧を高くせざるを得ず真空度低下検出時にはもは
やしや断できない真空度となつている、通電中
の常時真空度監視ができない。
D Problems to be Solved by the Invention As described above, in the conventional technology, as the degree of vacuum decreases, flashover occurs between the intermediate shield and both the fixed side and the movable side at approximately the same degree of vacuum. The load current cannot be cut off even if a drop in the vacuum level is detected.In order to avoid the effects of voltage fluctuations, the detection voltage must be increased, and when a drop in the vacuum level is detected, the vacuum level has reached such a level that it cannot be cut off anymore. It is not possible to constantly monitor the vacuum level while the power is on.

という問題点がある。There is a problem.

本発明はこのような問題点を解決するためにな
されたものである。
The present invention has been made to solve these problems.

E 問題点を解決するための手段 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6図に示す特性を得
た。第6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
6図中、実線m1、実線m2および実線m3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、A>B>Cの関係にある。
E. Means for Solving the Problems The present inventors studied the discharge phenomenon in a vacuum interrupter and obtained the characteristics shown in FIG. 6. FIG. 6 shows the vacuum interrupter internal pressure on the horizontal axis and the discharge starting voltage on the vertical axis. In FIG. 6, solid line m 1 , solid line m 2 and solid line m 3 indicate the characteristics of vacuum gaps A, B and C, respectively, and 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6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。そして、短ギヤ
ツプは、その10-2mmHg(1.333pa)前後の領域で
十分な耐電圧を保有していた。
It was generally known that long gaps have higher discharge starting voltages than short gaps, but as can be seen from Figure 6, this is a phenomenon in high vacuum or near atmospheric pressure, and is 10 -2 mmHg. In the region around (1.333pa), on the other hand, the discharge start voltage is higher in the gap than in the long gap. The short gap had sufficient withstand voltage in the region of around 10 -2 mmHg (1.333pa).

本発明はこのような知見にもとづき、先ず金属
性の中間シールドを電極に対し絶縁して設け、こ
の中間シールドと固定側又は可動側のいずれか一
方の系統電位部材との間に、真空度低下時であつ
てかつしや断可能領域で放電する真空ギヤツプを
形成する。そして系統電位部材例えば系統電路と
大地との間、及び中間シールドと大地との間に
夫々第1のインピーダンス及び第2のインピーダ
ンスを設けるとともに、第2のインピーダンスを
介して得た中間シールドの対地電位の検出信号を
前記真空インタラプタの開極時における検出信号
と閉極時における検出信号が真空度正常の場合に
等しくなるように補正する補正部と、該補正部に
よつて補正された信号と前記第1のインピーダン
スを介して得た系統電路の対地電位の検出信号と
を比較して真空度低下の有無を判定する判定部と
を設けて成る。
Based on this knowledge, the present invention first provides a metallic intermediate shield insulated from the electrode, and creates a space between the intermediate shield and the system potential member on either the fixed side or the movable side to reduce the degree of vacuum. Once in a while, a vacuum gap is formed that discharges in the area where it can be disconnected. Then, a first impedance and a second impedance are provided between the grid potential member, for example, between the grid line and the ground, and between the intermediate shield and the ground, respectively, and the ground potential of the intermediate shield obtained via the second impedance. a correction unit that corrects the detection signal of the vacuum interrupter so that the detection signal when the vacuum interrupter is open and the detection signal when the vacuum interrupter is closed are equal when the degree of vacuum is normal; A determination unit is provided that determines whether or not the degree of vacuum has decreased by comparing the detection signal of the ground potential of the system electric line obtained through the first impedance.

F 作用 上記のように構成された装置において、真空イ
ンタラプタの開極時における第2のインピーダン
スより得られる検出信号と閉極時における第2の
インピーダンスにより得られる検出信号とが真空
度正常の場合において等しくなるように、補正部
の補正量を設定しておく。これによつて真空度の
正常時に判定部に入力される中間シールドの対地
電圧検出量は、真空インタラプタの開極時も閉極
時も同じ値に補正される。この状態において通電
中(閉極時)に真空インタラプタの真空度が低下
してくると、しや断不能領域に至る前に固定側又
は可動側いずれか一方に設けている長ギヤツプの
部分で放電が始まる。この際他の真空ギヤツプ
(短ギヤツプ)では放電を生じず、短ギヤツプが
前記長ギヤツプの放電に誘発されて放電すること
はない。一方長ギヤツプで放電することにより、
中間シールドの対地電圧を閉極状態に対応した補
正量に基づいて補正した電位と系統電路の対地電
位との間の波高値差に変動が生じ、これによつて
判定部で真空度低下が直ちに検出される。そして
長ギヤツプのみが放電している段階で検出するの
で、その直後に電極を開極すれば電流をしや断す
ることができる。
F Effect In the device configured as described above, when the detection signal obtained from the second impedance when the vacuum interrupter is opened and the detection signal obtained from the second impedance when the vacuum interrupter is closed are normal in vacuum, The correction amount of the correction section is set so that they are equal. As a result, the detected amount of ground voltage of the intermediate shield, which is input to the determining section when the degree of vacuum is normal, is corrected to the same value both when the vacuum interrupter is opened and when it is closed. In this state, if the degree of vacuum in the vacuum interrupter decreases while energizing (when closed), a discharge occurs in the long gap provided on either the fixed side or the movable side before reaching the uninterruptable area. begins. At this time, no discharge occurs in the other vacuum gap (short gap), and the short gap is not induced to discharge by the discharge in the long gap. On the other hand, by discharging with a long gap,
A fluctuation occurs in the peak value difference between the potential of the intermediate shield that has been corrected based on the correction amount corresponding to the closed state and the ground potential of the grid circuit, and this causes the judgment unit to immediately detect a decrease in the degree of vacuum. Detected. Since it is detected when only the long gap is discharging, the current can be quickly cut off by opening the electrodes immediately after that.

また、開極中に真空インタラプタの真空度が低
下してくると、前記閉極時の場合と同様に長ギヤ
ツプの部分で放電が始まる。このため中間シール
ドの対地電位を開極状態に対応した補正量に基づ
いて補正した電位と系統電路の対地電位との間の
波高値差に変動が生じ、これによつて判定部で真
空度低下が直ちに検出される。
Furthermore, when the degree of vacuum in the vacuum interrupter decreases during opening, discharge begins in the long gap portion, similar to the case during closing. For this reason, a fluctuation occurs in the peak value difference between the ground potential of the intermediate shield corrected based on the correction amount corresponding to the open state and the ground potential of the grid circuit, and this causes a decrease in the degree of vacuum in the judgment section. is detected immediately.

G 実施例 以下、図面を参照しながら本発明の一実施例を
説明する。第1図において第8図と同一部分は同
一符号を持つて示し、その説明は省略する。この
実施例では、補助シールド3aの軸方向の長さを
小さくし、中間シールド2の固定端板41a側の
端部を補助シールド3aの端部よりも軸方向に十
分長く突出させて、その突出部分が補助シールド
3aをはさむことなくギヤツプを介して直接固定
電極棒4aと対向するように構成している。前記
ギヤツプのギヤツプ長lは、真空度低下時であつ
てしや断可能な真空領域で放電する長さであり、
真空インタラプタ1内の異電位部材間の最大距離
とされる。
G. Embodiment Hereinafter, an embodiment of the present invention will be described with reference to the drawings. In FIG. 1, the same parts as in FIG. 8 are indicated by the same reference numerals, and the explanation thereof will be omitted. In this embodiment, the axial length of the auxiliary shield 3a is made small, and the end of the intermediate shield 2 on the fixed end plate 41a side is made to protrude sufficiently longer than the end of the auxiliary shield 3a in the axial direction. The portion is configured to directly face the fixed electrode rod 4a via a gap without sandwiching the auxiliary shield 3a. The gap length l of the gap is a length that allows discharge in a vacuum region that can never be cut off when the degree of vacuum decreases,
This is the maximum distance between members of different potential within the vacuum interrupter 1.

尚異電位部材間で電子が飛行する場合、等電位
線と直交する方向に飛行するので、ここで述べる
距離とは電子の飛行距離を意味する。図中4bは
可動電極棒である。
Note that when electrons fly between members with different potentials, they fly in a direction perpendicular to the equipotential lines, so the distance described here means the flight distance of the electrons. In the figure, 4b is a movable electrode rod.

5は、系統電路の対地電位E1を検出する第1
のインピーダンス分圧器であり、例えば真空イン
タラプタ1の近傍において電源側電路と大地との
間に設けられている。この第1のインピーダンス
分圧器5は、コンデンサや抵抗等のインピーダン
ス成分Z1,Z2により構成される。
5 is a first circuit that detects the ground potential E1 of the grid line.
This is an impedance voltage divider, and is provided, for example, in the vicinity of the vacuum interrupter 1 between the power supply side electric circuit and the ground. The first impedance voltage divider 5 is composed of impedance components Z 1 and Z 2 such as capacitors and resistors.

6は中間シールド2の対地電位E3を検出する
第2のインピーダンス分圧器であり、例えば容量
が夫々0.1μF,1000pFのコンデンサC1,C2で構成
される。尚第2のインピーダンス分圧器6はコン
デンサを用いることに限定されるものではない。
7は負荷を示している。上記のような構造の真空
インタラプタ1に第1および第2インピーダンス
分圧器5,6を設けた場合の等価回路は第2図に
示される。第2図においてC4は中間シールド2
と可動電極4bの間の容量を各々示している。第
1図および第2図では閉極状態を表わしている
が、開極時の回路は第3図および第4図のように
示される。これらの図において8は真空インタラ
プタ1の開極時に負荷7の両端を短絡させるため
の設置装置であり、C5は電極間容量を示してい
る。閉極時を示す第2図の等価回路において、検
出電圧e3は次式のような分圧比で求められる。
6 is a second impedance voltage divider for detecting the ground potential E 3 of the intermediate shield 2, and is composed of capacitors C 1 and C 2 with capacitances of 0.1 μF and 1000 pF, respectively. Note that the second impedance voltage divider 6 is not limited to using a capacitor.
7 indicates the load. FIG. 2 shows an equivalent circuit when the vacuum interrupter 1 having the above structure is provided with the first and second impedance voltage dividers 5 and 6. In Figure 2, C 4 is intermediate shield 2
and the movable electrode 4b. Although FIGS. 1 and 2 show the closed state, the circuit when the contacts are open is shown in FIGS. 3 and 4. In these figures, 8 is an installation device for short-circuiting both ends of the load 7 when the vacuum interrupter 1 is opened, and C 5 indicates the interelectrode capacitance. In the equivalent circuit of FIG. 2 showing the closed pole, the detected voltage e 3 is determined by the voltage division ratio as shown in the following equation.

e3 =1/C1/(1/C1)+(1/C2)+{1/(C3+C4
)} ……(1) また開極時を示す第4図の等価回路において、
検出電圧e3は次式のような分圧比で求められる。
e 3 = 1/C 1 / (1/C 1 ) + (1/C 2 ) + {1/(C 3 +C 4
)} ...(1) Also, in the equivalent circuit of Fig. 4 showing the open circuit,
The detection voltage e 3 is determined by the voltage division ratio as shown in the following equation.

e3=1/C1/1/C1+1/C2+1/C3+C3(C4+C5
/C3+C4+C5……(2) 第2図および第4図の等価回路からわかるよう
に真空インタラプタ1の閉極時におけるインピー
ダンス分圧器6の検出電圧e3と開極時における検
出電圧e3は互いに異なる電圧値となる。このため
本発明では電圧補正部9によつて中間シールド2
の対地電圧E3に比例した検出電圧e3(第2のイン
ピーダンス分圧器6の出力電圧)を真空インタラ
プタ1の開閉状態に応じて次のように補正する。
すなわち電圧補正部9の10は、しや断器の補助
開閉器であり、該補助開閉器10は真空インタラ
プタ1の開閉状態の検出信号を増幅率決定回路1
1に送出する。12は接地装置8の補助リレーで
ある。接地装置8のON又はOFF状態の検出信号
を増幅率決定回路11に送出する。尚補助リレー
12は第1図のように接地装置8を設けない場合
は省略できる。増幅率決定回路11は、前記補助
開閉器10および補助リレー12の検出信号(開
閉状態を表わす信号)に応じて前置増幅器13の
増幅率を決定する回路であり、例えば予め設定し
た複数の増幅率から前記検出信号に応じた増幅率
を選択するように構成されている。前置増幅器1
3は増幅率決定回路11で決定された増幅率によ
り第2のインピーダンス分圧器6の検出電圧e3
増幅する。このように真空インタラプタ1の開閉
状態に応じて決定された増幅率で増幅することに
より前記検出電圧e3が補正されるので、閉極時の
検出電圧e3を前置増幅器13によつて増幅した電
圧e3′と開極時の検出電圧e3を前置増幅器13に
よつて増幅した電圧e3″とを等しくすることがで
きる。14は判定部であり、この判定部14は第
1のインピーダンス分圧器5の検出電圧e1と前置
増幅器13の出力電圧e3′,E3″との波高値差を増
幅する差動増幅器15と、この差動増幅器15の
偏差出力と前記補助開閉器10および補助リレー
12の出力信号と電源電圧の有無を検出する電圧
検出器16の検出信号とに基づいて真空度低下を
判定する判定回路17とで構成されている。判定
回路17は、差動増幅器15の偏差出力が所定値
以上になつたとき真空度低下の判定信号、例えば
警報を発するとともに、電源電圧検出器16が無
電圧を検出したとき前記警報の発生を阻止して表
示器(図示省略)に電源電圧無しの表示を行なわ
せる機能を有している。
e 3 = 1/C 1 /1/C 1 +1/C 2 +1/C 3 +C 3 (C 4 +C 5 )
/C 3 +C 4 +C 5 ...(2) As can be seen from the equivalent circuits in Figures 2 and 4, the detected voltage e 3 of the impedance voltage divider 6 when the vacuum interrupter 1 is closed and the detected voltage when the vacuum interrupter 1 is opened e 3 have different voltage values. Therefore, in the present invention, the intermediate shield 2
The detected voltage e 3 ( output voltage of the second impedance voltage divider 6) proportional to the ground voltage E 3 of is corrected as follows according to the open/closed state of the vacuum interrupter 1.
In other words, 10 of the voltage correction section 9 is an auxiliary switch for the breaker, and the auxiliary switch 10 converts the detection signal of the open/closed state of the vacuum interrupter 1 into the amplification factor determining circuit 1.
Send to 1. 12 is an auxiliary relay of the grounding device 8. A detection signal indicating the ON or OFF state of the grounding device 8 is sent to the amplification factor determining circuit 11. The auxiliary relay 12 can be omitted if the grounding device 8 is not provided as shown in FIG. The amplification factor determination circuit 11 is a circuit that determines the amplification factor of the preamplifier 13 according to the detection signals (signals representing the open/closed state) of the auxiliary switch 10 and the auxiliary relay 12, and for example, the amplification factor of the preamplifier 13 is The amplification factor is selected from the amplification factor according to the detection signal. Preamplifier 1
3 amplifies the detected voltage e 3 of the second impedance voltage divider 6 by the amplification factor determined by the amplification factor determination circuit 11. Since the detected voltage e 3 is corrected by amplifying with the amplification factor determined according to the open/closed state of the vacuum interrupter 1, the detected voltage e 3 when the pole is closed is amplified by the preamplifier 13. It is possible to make equal the voltage e 3 ′ obtained by amplifying the detected voltage e 3 at the time of opening by the preamplifier 13. 14 is a determination unit, and this determination unit 14 A differential amplifier 15 amplifies the peak value difference between the detected voltage e 1 of the impedance voltage divider 5 and the output voltages e 3 ′, E 3 ″ of the preamplifier 13; It is comprised of a determination circuit 17 that determines a decrease in the degree of vacuum based on the output signals of the switch 10 and the auxiliary relay 12 and the detection signal of the voltage detector 16 that detects the presence or absence of power supply voltage. The determination circuit 17 issues a determination signal, for example, an alarm, for a decrease in the degree of vacuum when the deviation output of the differential amplifier 15 exceeds a predetermined value, and also issues an alarm when the power supply voltage detector 16 detects no voltage. It has a function of blocking the voltage and causing a display (not shown) to display that there is no power supply voltage.

次に上記実施例の作用について述べる。系統線
路電圧および中間シールド電圧は各々インピーダ
ンス分圧器5,6で検出され、その検出電圧e1
差動増幅器15に入力されるとともに、検出電圧
e3は前置増幅器13によつて真空インタラプタ1
の開閉状態に応じた増幅率で増幅された後、差動
増幅器15に入力される。真空度が正常なときに
は検出電圧e1と前置増幅器13の出力電圧e3′,
e3″との間には所定の波高値差があり、差動増幅
器15からその偏差に対応する信号が出力されて
いる。このとき判定回路17からは真空度低下の
判定信号は出力されない。ここで真空度が低下す
ると、中間シールド2と固定電極棒4aとの間の
ギヤツプにて放電し始める。その理由は、第6図
に示したパツシエンカーブの10-2mmHg(1.333Pa)
前後の領域では、ギヤツプ長が大きいところから
放電する特性になつており、前記ギヤツプ長lは
真空インタラプタ1内の異電位部材間の最大距離
とされているため、このギヤツプにて最初に局部
的に放電し始めるのである。この結果中間シール
ド2の電位が変化して、検出電圧e1と前置増幅器
13の出力電圧e3′,e3″との間の波高値差が変化
し、その変化分が所定の大きさを越えると判定回
路17から真空度低下の判定信号が出力される。
尚、第5図は真空度が低下したときの各検出電位
の波形図である。
Next, the operation of the above embodiment will be described. The grid line voltage and the intermediate shield voltage are detected by impedance voltage dividers 5 and 6, respectively, and the detected voltage e1 is input to the differential amplifier 15, and the detected voltage
e 3 is connected to vacuum interrupter 1 by preamplifier 13.
After being amplified with an amplification factor according to the open/closed state of the signal, the signal is input to the differential amplifier 15. When the degree of vacuum is normal, the detection voltage e 1 and the output voltage e 3 ' of the preamplifier 13,
There is a predetermined peak value difference between e 3 ″ and the differential amplifier 15 outputs a signal corresponding to the deviation. At this time, the determination circuit 17 does not output a determination signal for a decrease in the degree of vacuum. When the degree of vacuum decreases, discharge begins in the gap between the intermediate shield 2 and the fixed electrode rod 4a.The reason for this is 10 -2 mmHg (1.333 Pa) of the Passien curve shown in Figure 6.
In the front and rear regions, the discharge occurs from a place where the gap length is large, and since the gap length l is the maximum distance between members with different potentials in the vacuum interrupter 1, the discharge occurs locally in this gap first. It begins to discharge. As a result, the potential of the intermediate shield 2 changes, and the peak value difference between the detection voltage e 1 and the output voltages e 3 ′ and e 3 ″ of the preamplifier 13 changes, and the amount of the change increases to a predetermined magnitude. When the value exceeds the threshold, the determination circuit 17 outputs a determination signal indicating a decrease in the degree of vacuum.
Incidentally, FIG. 5 is a waveform diagram of each detected potential when the degree of vacuum decreases.

以上のように上記実施例の判定回路17は、電
源電圧検出器16が無電圧を検出したとき真空度
低下の警報の発生を阻止する機能を有しているの
で、誤つた警報が発せられることは無い。
As described above, the determination circuit 17 of the above embodiment has a function of preventing the generation of a vacuum level lowering alarm when the power supply voltage detector 16 detects no voltage, so that a false alarm may not be issued. There is no.

尚、上記実施例では、固定電極部4aと中間シ
ールド2との間に前記最大距離をもつたギヤツプ
を設けているが、本発明では固定側及び可動側で
の閃絡を避けることから固定側又は可動側のいず
れか一方であれば、電極棒に限らず金属端板41
a,41b等の系統電位部材と中間シールド2と
の間に、真空度低下時であつてかつしや断可能な
真空領域で放電する真空ギヤツプを設ける構成と
してもよい。
In the above embodiment, a gap having the maximum distance is provided between the fixed electrode part 4a and the intermediate shield 2, but in the present invention, in order to avoid flashover on the fixed side and the movable side, the gap on the fixed side is Or if it is either the movable side, it is not limited to the electrode rod, but the metal end plate 41
A vacuum gap may be provided between the system potential members such as a and 41b and the intermediate shield 2, which discharges in a vacuum region that can be cut off when the degree of vacuum is reduced.

H 発明の効果 以上のように本発明によれば、中間シールドと
固定側又は可動側のいずれか一方の系統電位部材
との間に、真空度低下時であつてかつしや断可能
領域で放電する真空ギヤツプを形成しているの
で、真空度低下のリーク初期(高真空)時に固定
側か可動側かの一方で放電を生じる。この際、他
の真空ギヤツプは十分な耐電圧を保有している。
しかも中間シールドの対地電位の検出信号を真空
インタラプタの開閉状態に応じて補正した信号と
系統電位部材の対地電位の検出信号とを波高値に
ついて比較し、波高値差の変化を捉えて真空度低
下を検出する構成であるため、系統電路の電圧変
動や重量ノイズによる影響を受けることなく、真
空度低下による局部放電の段階で検出することが
できる。この結果、真空度低下のリーク初期時を
捉えることができるので使用電圧範囲(しや断可
能電圧)よりも高い耐圧をもつた真空度領域で対
応でき、真空度低下の検出後にしや断することが
できる。
H. Effects of the Invention As described above, according to the present invention, a discharge occurs between the intermediate shield and the grid potential member on either the fixed side or the movable side in a region where the degree of vacuum is reduced and it is possible to Since a vacuum gap is formed, an electric discharge occurs on either the fixed side or the movable side at the beginning of a leak (high vacuum) when the degree of vacuum decreases. At this time, the other vacuum gaps have sufficient withstand voltage.
In addition, the signal obtained by correcting the detection signal of the ground potential of the intermediate shield according to the open/closed state of the vacuum interrupter is compared with the detection signal of the ground potential of the grid potential member in terms of peak value, and the degree of vacuum is reduced by capturing the change in the peak value difference. Since it is configured to detect this, it can be detected at the stage of local discharge due to a decrease in the degree of vacuum without being affected by voltage fluctuations in the grid circuit or weight noise. As a result, it is possible to detect the initial stage of a leak due to a decrease in vacuum level, so it is possible to respond in a vacuum range with a higher withstand voltage than the operating voltage range (voltage that can be interrupted), and it can be interrupted after detecting a decrease in vacuum level. be able to.

また中間シールドの対地電位の検出信号を真空
インタラプタの開閉状態に応じて補正しているた
め、開極時および閉極時における中間シールドの
対地電位の検出信号を互いに等しくすることがで
きる。これによつて開極、閉極のいずれの状態で
あつても真空度低下を正確に判定することができ
る。このため真空インタラプタの開閉動作が繰り
返して行なわれる場合であつても常時真空度監視
ができる。
Further, since the detection signal of the ground potential of the intermediate shield is corrected according to the open/closed state of the vacuum interrupter, the detection signals of the ground potential of the intermediate shield can be made equal when the contact is opened and when the contact is closed. This makes it possible to accurately determine the decrease in the degree of vacuum in either the open or closed state. Therefore, even if the vacuum interrupter is repeatedly opened and closed, the degree of vacuum can be constantly monitored.

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

第1図は本発明の実施例を示す回路図、第2図
は第1図の回路と等価回路を示す回路図、第3図
は本発明の実施例の要部回路図、第4図は第3図
の回路と等価回路を示す回路図、第5図は各イン
ピーダンス検出器よりの検出電位を示す波形図、
第6図は真空ギヤツプが異なる場合の真空度とギ
ヤツプ間の放電開始電圧との関係を示す曲線図、
第7図はパツシエンの法則を示す曲線図、第8
図、第9図は各々従来の真空度低下検出装置の原
理を示す原理図である。 1……真空インタラプタ、2……中間シール
ド、3a,3b……補助シールド、4a……固定
電極棒、4b……可動電極棒、5……第1のイン
ピーダンス分圧器、6……第2のインピーダンス
分圧器、7……負荷、8……接地装置、9……電
圧補正部、10……しや断器の補助開閉器、11
……増幅率決定回路、12……補助リレー、13
……前置増幅器、14……判定部、15……差動
増幅器、16……電圧検出器、17……判定回
路。
Fig. 1 is a circuit diagram showing an embodiment of the present invention, Fig. 2 is a circuit diagram showing an equivalent circuit to the circuit in Fig. 1, Fig. 3 is a main part circuit diagram of the embodiment of the invention, and Fig. 4 is A circuit diagram showing an equivalent circuit to the circuit in Fig. 3, and Fig. 5 a waveform diagram showing detected potentials from each impedance detector.
Fig. 6 is a curve diagram showing the relationship between the degree of vacuum and the discharge starting voltage between the gaps when the vacuum gap is different;
Figure 7 is a curve diagram showing Patsien's law, Figure 8
9 are principle diagrams showing the principle of a conventional vacuum level drop detection device. DESCRIPTION OF SYMBOLS 1... Vacuum interrupter, 2... Intermediate shield, 3a, 3b... Auxiliary shield, 4a... Fixed electrode bar, 4b... Movable electrode bar, 5... First impedance voltage divider, 6... Second Impedance voltage divider, 7...Load, 8...Grounding device, 9...Voltage correction section, 10...Auxiliary switch for breaker, 11
...Amplification factor determination circuit, 12...Auxiliary relay, 13
... Preamplifier, 14 ... Judgment section, 15 ... Differential amplifier, 16 ... Voltage detector, 17 ... Judgment circuit.

Claims (1)

【特許請求の範囲】 1 筒体の両端を端板で閉塞して真空容器を形成
し、この真空容器に一方の端板から固定電極棒を
気密に導入しかつ他方の端板から固定電極棒に接
近離反自在の可動電極棒をベローズを介して気密
に導入し、これら両電極棒の各内端部に対をなし
て接離自在の固定、可動電極を設けるとともに、 真空容器内に少なくとも前記電極の外周を囲繞
する金属製の中間シールドを電極に対し絶縁して
設けて成る系統電路開閉自在の真空インタラプタ
の真空度低下を検出する装置において、 前記中間シールドと固定側又は可動側のいずれ
か一方の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領域で放電する真空
ギヤツプを形成し、系統電位部材と大地との間に
設けられた第1のインピーダンスと、前記中間シ
ールドと大地との間に設けられた第2のインピー
ダンスと、この第2のインピーダンスを介して得
た中間シールドの対地電位の検出信号を、前記真
空インタラプタの開極時における検出信号と閉極
時における検出信号が真空度正常の場合に等しく
なるように補正する補正部と、この補正部によつ
て補正された信号と前記第1のインピーダンスを
介して得た系統電位部材の対地電位の検出信号と
を比較して真空度低下の有無を判定する判定部と
を有して成る真空インタラプタの真空度低下検出
装置。
[Scope of Claims] 1. A vacuum container is formed by closing both ends of a cylinder with end plates, and a fixed electrode rod is airtightly introduced into the vacuum container from one end plate, and a fixed electrode rod is inserted from the other end plate. A movable electrode rod that can be moved toward and away from the electrode is airtightly introduced through a bellows, and a pair of fixed and movable electrodes that can be moved toward and away from each other is provided at each inner end of these electrode rods, and at least the above-mentioned In a device for detecting a decrease in the degree of vacuum in a vacuum interrupter capable of freely opening and closing a power grid circuit, the intermediate shield made of metal surrounding the outer periphery of an electrode is provided insulated from the electrode, the intermediate shield and either a fixed side or a movable side. A first impedance is provided between the grid potential member and the ground, forming a vacuum gap that discharges in a vacuum region that can be disconnected when the degree of vacuum is reduced, and the grid potential member and the ground. and a second impedance provided between the intermediate shield and the ground, and a detection signal of the ground potential of the intermediate shield obtained through the second impedance when the vacuum interrupter is opened. and a correction unit that corrects the detection signal when the pole is closed to be equal to that when the degree of vacuum is normal, and the signal corrected by the correction unit and the ground potential of the grid potential member obtained through the first impedance. A device for detecting a decrease in the degree of vacuum of a vacuum interrupter, comprising a determination unit that determines whether there is a decrease in the degree of vacuum by comparing the detection signal with a potential detection signal.
JP13748485A 1985-06-24 1985-06-24 Vacuum drop detector for vacuum interruptor Granted JPS61294725A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13748485A JPS61294725A (en) 1985-06-24 1985-06-24 Vacuum drop detector for vacuum interruptor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13748485A JPS61294725A (en) 1985-06-24 1985-06-24 Vacuum drop detector for vacuum interruptor

Publications (2)

Publication Number Publication Date
JPS61294725A JPS61294725A (en) 1986-12-25
JPH0434247B2 true JPH0434247B2 (en) 1992-06-05

Family

ID=15199712

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13748485A Granted JPS61294725A (en) 1985-06-24 1985-06-24 Vacuum drop detector for vacuum interruptor

Country Status (1)

Country Link
JP (1) JPS61294725A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
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
JP5020273B2 (en) * 2009-02-24 2012-09-05 中国電力株式会社 Vacuum circuit breaker Vacuum tester

Also Published As

Publication number Publication date
JPS61294725A (en) 1986-12-25

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