JPS645648B2 - - Google Patents
Info
- Publication number
- JPS645648B2 JPS645648B2 JP1267482A JP1267482A JPS645648B2 JP S645648 B2 JPS645648 B2 JP S645648B2 JP 1267482 A JP1267482 A JP 1267482A JP 1267482 A JP1267482 A JP 1267482A JP S645648 B2 JPS645648 B2 JP S645648B2
- Authority
- JP
- Japan
- Prior art keywords
- vacuum
- shield
- disconnector
- antenna
- signal
- 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
Links
- 238000012806 monitoring device Methods 0.000 claims description 10
- 230000006866 deterioration Effects 0.000 description 13
- 239000004020 conductor Substances 0.000 description 9
- 238000001514 detection method Methods 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 4
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- 229910052751 metal Inorganic materials 0.000 description 3
- 239000002243 precursor Substances 0.000 description 3
- 230000035945 sensitivity Effects 0.000 description 3
- 125000000391 vinyl group Chemical group [H]C([*])=C([H])[H] 0.000 description 3
- 229920002554 vinyl polymer Polymers 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005219 brazing Methods 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 238000003466 welding Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L21/00—Vacuum gauges
- G01L21/30—Vacuum gauges by making use of ionisation effects
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H33/00—High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
- H01H33/60—Switches wherein the means for extinguishing or preventing the arc do not include separate means for obtaining or increasing flow of arc-extinguishing fluid
- H01H33/66—Vacuum switches
- H01H33/668—Means for obtaining or monitoring the vacuum
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Examining Or Testing Airtightness (AREA)
- Measuring Fluid Pressure (AREA)
Description
【発明の詳細な説明】
本発明は真空しや断器の真空度監視装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum degree monitoring device for a vacuum shield breaker.
一般に真空しや断器はその真空度が10-4Torr
以下の圧力で正常なしや断能力を有しているが、
この真空度はしや断器内部からの放出ガスや溶接
およびろう付けなどの接合部からのスローリーク
などによつて劣化し、しや断能力が低下すること
がある。このため、真空しや断器の使用時におい
てはその真空度を監視することが性能保証上から
必要欠くべからざるものとなつている。 Generally, the vacuum degree of a vacuum disconnector is 10 -4 Torr.
It is normal or has the ability to break at pressures below,
This vacuum level may deteriorate due to gas released from inside the breaker or disconnector, or slow leakage from joints such as welding and brazing, resulting in a decrease in breaker ability. For this reason, when using a vacuum chamber or disconnector, it is essential to monitor the degree of vacuum in order to guarantee performance.
そこで従来においては、真空しや断器内部に放
電電極を設けるとともに別電源により高電圧を印
加し、この際のパツシエンの法測による放電状態
が真空度により変化することを利用して真空度の
チエツクを行うなどしていたが、このような方法
では真空しや断器の構造が複雑になるとともに高
電圧の別電源を用意しなければならないため高価
になつた。又、真空度のチエツクに際しては真空
しや断器を回路から切離した場合は真空しや断器
の可動電極を固定電極から真空度劣化によるパツ
シエンの法則に依存される。放電し易い距離だけ
開極して、別電源から高電圧を印加し、この際の
放電状態により真空度の良否を判定していた。こ
の方法では電源を止める必要もあり、非常に面倒
であつた。 Conventionally, a discharge electrode is provided inside the vacuum chamber or disconnector, and a high voltage is applied from a separate power supply. At this time, the discharge state according to Patsien's method changes depending on the degree of vacuum, and this is used to control the degree of vacuum. However, this method complicated the structure of the vacuum shield and disconnector, and required a separate high-voltage power source, making it expensive. Furthermore, when checking the degree of vacuum, if the vacuum shield or breaker is disconnected from the circuit, the movable electrode of the vacuum shield or breaker is replaced by the fixed electrode depending on Patsien's law due to the deterioration of the vacuum degree. The electrodes were opened to a distance that facilitated discharge, and a high voltage was applied from a separate power source, and the quality of the vacuum was determined based on the discharge state at this time. This method required turning off the power, which was very troublesome.
本発明は上記の欠点を除去して、放電電極や高
電圧の別電源を必要とせず、かつ真空しや断器を
回路に接続したままその真空度のチエツクを行う
ことができ、真空度のチエツクを簡単かつ安価に
行うことができる真空しや断器の真空度監視装置
を提供することを目的とする。 The present invention eliminates the above-mentioned drawbacks, does not require a discharge electrode or a separate high-voltage power source, and can check the vacuum level of a vacuum shield or disconnector while it is connected to the circuit. It is an object of the present invention to provide a vacuum level monitoring device for a vacuum shield or disconnector that can be checked easily and inexpensively.
以下本発明の図面とともに説明する。第1図に
おいて、1は真空しや断器で、真空しや断器1は
絶縁筒2の両端に金属製の端板3,4を取付けて
真空容器を形成し、端板3には固定リード5を挿
着するとともに端板4にはベローズ6を介して可
動リード7を移動可能に挿着し、固定リード5お
よび可動リード7の先端には夫々固定電極8およ
び可動電極9を取付ける。又、絶縁筒2の中間に
はしや断時電極8,9間に発生する金属蒸気が絶
縁筒2の内面に付着するのを防止するためのシー
ルド10を取付ける。11,12は補助シール
ド、13,14は外部接続導体、15は集電部で
ある。16は真空しや断器1の近傍に配設される
べき電磁波信号受信部材、たとえばアンテナで、
このアンテナ16は接続線17により検出器18
に接続されている。検出器18は増幅器19、判
定部20、電源部21および表示部22から構成
されている。 The present invention will be explained below with reference to the drawings. In Fig. 1, 1 is a vacuum shield disconnector.The vacuum shield disconnector 1 has metal end plates 3 and 4 attached to both ends of an insulating cylinder 2 to form a vacuum container, and is fixed to the end plate 3. While the lead 5 is inserted, a movable lead 7 is movably inserted into the end plate 4 via a bellows 6, and a fixed electrode 8 and a movable electrode 9 are attached to the tips of the fixed lead 5 and the movable lead 7, respectively. Further, a shield 10 is installed in the middle of the insulating cylinder 2 to prevent metal vapor generated between the chopping electrodes 8 and 9 from adhering to the inner surface of the insulating cylinder 2. 11 and 12 are auxiliary shields, 13 and 14 are external connection conductors, and 15 is a current collector. 16 is an electromagnetic wave signal receiving member, such as an antenna, to be disposed near the vacuum shield breaker 1;
This antenna 16 is connected to a detector 18 by a connecting line 17.
It is connected to the. The detector 18 includes an amplifier 19, a determination section 20, a power supply section 21, and a display section 22.
第2図Aは検出器18の詳細を示すブロツク図
で、23はアンテナ16で検出した検出信号を増
幅するバツフアアンプ、24はバツフアアンプ2
3の出力信号(第2図Bに示すS1)から2〜20k
Hzの周波数成分のみを通過させるバンドパスフイ
ルタである。このバンドパスフイルタ24の出力
信号(第2図Bに示すS2)はアンプ25により増
幅され、この増幅出力信号(第2図Bに示すS3)
は第1の比較器26に入力されて所定の基準電圧
と比較される。第1の比較器26の出力信号(第
2図Bに示すS4)は積分器27で積分され、この
積分出力信号(第2図Bに示すS5)は第2の比較
器28に入力されて第2の比較器28の所定の基
準電圧と比較され、その出力に第2図Bに示すS6
の信号を送出する。この信号は警報及び表示信号
となる。 FIG. 2A is a block diagram showing details of the detector 18, in which 23 is a buffer amplifier that amplifies the detection signal detected by the antenna 16, and 24 is a buffer amplifier 2.
2 to 20k from the output signal of 3 (S 1 shown in Figure 2B)
This is a bandpass filter that passes only Hz frequency components. The output signal (S 2 shown in FIG. 2B) of this bandpass filter 24 is amplified by the amplifier 25, and this amplified output signal (S 3 shown in FIG. 2B)
is input to the first comparator 26 and compared with a predetermined reference voltage. The output signal of the first comparator 26 (S 4 shown in FIG. 2B) is integrated by an integrator 27, and this integrated output signal (S 5 shown in FIG. 2B) is input to the second comparator 28. is compared with a predetermined reference voltage of the second comparator 28, and the output is S 6 as shown in FIG. 2B.
The signal is sent out. This signal becomes an alarm and display signal.
上記構成において、真空しや断器1は図示しな
い操作装置により可動リード7を動かし、電極
8,9を接離して投入し,しや断を行うが真空し
や断器1のしや断状態における等価回路図を第3
図に示す。図において、28,29は夫々真空し
や断器1の設置された回路の電源および負荷、3
0,31は夫々固定リード5の真空容器内の部分
および固定電極8とシールド10間の抵抗および
静電容量、32,33は夫々可動リード7の真空
容器内の部分および可動電極9とシールド10間
の抵抗および静電容量、34a,34bは夫々絶
縁筒2の抵抗、35はシールド10と大地間の静
電容量、36,37は夫々しや断状態における電
極8,9間の抵抗および静電容量である。真空し
や断器1の内部の真空度が劣化した場合即ち内部
圧力が上昇した場合、真空中の誘電率と大気中の
誘電率がほぼ等しいために静電容量31,33,
37はほとんど変化しないが、抵抗30,32,
36はパツシエンの法則に影響される前駆現象に
より著しく低下する。このため、絶縁筒2により
固定側および可動側のいずれとも絶縁され、浮遊
電位を有するシールド10と各電極8,9との間
においては投入状態およびしや断状態にかかわら
ず放電が生じ、又電極8,9間においてはしや断
状態においてのみ放電が生じる。この放電は負荷
側にケーブル(静電容量)接続,誘導負荷線ある
いは真空しや断器のリードの静電容量によつて変
化する。 In the above configuration, the vacuum sheath breaker 1 moves the movable lead 7 by an operating device (not shown), connects and separates the electrodes 8 and 9, and disconnects the sheath, but the vacuum sheath breaker 1 is in a sheared state. The equivalent circuit diagram for
As shown in the figure. In the figure, 28 and 29 are the power supply and load of the circuit in which the vacuum shield breaker 1 is installed, and 3
0 and 31 are the resistance and capacitance between the portion of the fixed lead 5 inside the vacuum container and the fixed electrode 8 and the shield 10, respectively; 32 and 33 are the portion of the movable lead 7 inside the vacuum container and the movable electrode 9 and the shield 10, respectively. 34a and 34b are the resistances of the insulating cylinder 2, 35 is the capacitance between the shield 10 and the ground, and 36 and 37 are the resistances and capacitances between the electrodes 8 and 9 in the disconnected state, respectively. It is the capacitance. When the degree of vacuum inside the vacuum chamber breaker 1 deteriorates, that is, when the internal pressure increases, the capacitances 31, 33,
37 hardly changes, but the resistances 30, 32,
36 is significantly reduced by a precursor phenomenon influenced by Patsien's law. Therefore, discharge occurs between the shield 10, which is insulated from both the fixed side and the movable side by the insulating tube 2 and has a floating potential, and each electrode 8, 9, regardless of whether it is in the closed state or the shrunk state. Discharge occurs between the electrodes 8 and 9 only in the disconnected state. This discharge changes depending on the cable (capacitance) connection on the load side, the inductive load line, or the capacitance of the vacuum shield or disconnector lead.
第4図Aは真空しや断器1の真空度が正常なと
きの電極間電圧を示し、第4図Bはアンテナ16
による受信信号を示す。すなわち真空度が正常な
ときは、第4図Aに示すように電極8,9間の電
圧波形は正弦波であり、アンテナ16には真空し
や断器以外の回転機、変圧器、計器などから発生
すると思われる2kHz以下の高調波を含む信号が
入力される。第5図AおよびBは真空しや断器1
の真空度が劣化した場合の極間電圧およびアンテ
ナ16の受信信号を示し、電極8と9間の極間電
圧は、放電が始まると、第5図Aに示すようにあ
る電圧以上には上昇せずリツプルする。このリツ
プル開始時に第5図Bに示すように2〜20kHzの
高周波を含む電磁波信号が発生し、この信号を検
出し、判定することにより真空しや断器1の真空
度劣化を検知できる。この場合、真空しや断器以
外の他の部分でコロナ放電が発生しても信号波形
は異なるため検出特性には何ら影響がない。 Figure 4A shows the voltage between the electrodes when the degree of vacuum in the vacuum shield breaker 1 is normal, and Figure 4B shows the voltage between the antennas 16 and 16.
The received signal is shown below. That is, when the degree of vacuum is normal, the voltage waveform between the electrodes 8 and 9 is a sine wave as shown in FIG. A signal containing harmonics of 2kHz or less, which are thought to be generated from Figure 5 A and B are vacuum shield disconnector 1
The voltage between electrodes 8 and 9 and the received signal of antenna 16 are shown when the degree of vacuum deteriorates, and when the discharge starts, the voltage between electrodes 8 and 9 rises above a certain voltage as shown in Figure 5A. Ripple without. At the start of this ripple, an electromagnetic wave signal containing a high frequency of 2 to 20 kHz is generated as shown in FIG. In this case, even if corona discharge occurs in other parts than the vacuum chamber or the disconnector, the signal waveform will be different, so there will be no effect on the detection characteristics.
真空しや断器1の真空度が劣化時において、ア
ンテナ16が電磁波信号を受信する。真空度を5
×10-3〜300Torr間で変えて測定した電磁波は負
荷側の大地間静電容量が0.0042μFの時10〜14K
Hz、0.05μFの時2〜8kHz、0.2μF又は0.2μF以上
の時2〜20kHzの周波数を含んでおり、0.0042μF
の時の電磁波の波形はパルス的であつた。負荷側
の静電容量が0.0042μF以下と小さい時は電磁波の
検出感度が不安定となるので0.2μF程度の静電容
量を大地間に接続すればよい。第2図A,Bに示
すようにバツフアアンプ23はこれを増幅して出
力信号S1を送出する。この出力信号S1はバンドパ
スフイルタ24に入力され、その信号中2〜20k
Hzの周波数成分のみがフイルタ24から出力され
る。この出力信号S2はアンプ25により増幅され
る。この増幅信号S3は第1の比較器26に入力さ
れる。第1の比較器26においては、信号S3と所
定の基準電圧とを比較して信号S4を積分器27に
入力する。積分器27は第1の比較器26の偏差
信号を積分して出力信号S5を第2の比較器28に
入力する。第2の比較器28は信号S5を所定の基
準電圧と比較してその偏差電圧信号S6を出力し警
報器または表示器を動作させ、真空度劣化が検出
される。 When the degree of vacuum in the vacuum shield breaker 1 deteriorates, the antenna 16 receives an electromagnetic wave signal. Vacuum level 5
The electromagnetic waves measured by changing between ×10 -3 and 300Torr are 10 to 14K when the ground capacitance on the load side is 0.0042μF.
Hz, includes frequencies of 2 to 8kHz when 0.05μF, 2 to 20kHz when 0.2μF or 0.2μF or more, 0.0042μF
The waveform of the electromagnetic waves at this time was pulse-like. When the capacitance on the load side is as small as 0.0042 μF or less, the electromagnetic wave detection sensitivity becomes unstable, so a capacitance of about 0.2 μF should be connected to the ground. As shown in FIGS. 2A and 2B, the buffer amplifier 23 amplifies this and sends out an output signal S1 . This output signal S1 is input to the band pass filter 24, and 2 to 20 k
Only the Hz frequency component is output from the filter 24. This output signal S 2 is amplified by an amplifier 25. This amplified signal S 3 is input to the first comparator 26 . The first comparator 26 compares the signal S 3 with a predetermined reference voltage and inputs the signal S 4 to the integrator 27 . The integrator 27 integrates the deviation signal of the first comparator 26 and inputs the output signal S 5 to the second comparator 28 . The second comparator 28 compares the signal S 5 with a predetermined reference voltage and outputs a deviation voltage signal S 6 to operate an alarm or indicator, and deterioration of the degree of vacuum is detected.
実験測定結果によれば、長さが30cm、断面積
1.25mm2のビニール被覆銅線ケーブルをアンテナ1
6に使用したとき、1m離れた位置にある真空度
10-1Torr程度の6.9kV用真空しや断器の開極時に
負荷側に0.2μFの静電容量を大地間に接続し例え
ば6.9/√3≒4kVの電圧を印加すると電極間に
て放電した。これを上記アンテナ16にて捕え検
出器18に入力すると、増幅器からの信号はゲイ
ンが10000のとき0.6Vの振れ幅となつた。 According to the experimental measurement results, the length is 30cm, the cross-sectional area
Connect the 1.25mm 2 vinyl coated copper cable to antenna 1.
6, the degree of vacuum at a distance of 1m
When a 6.9kV vacuum shield circuit breaker with a voltage of about 10 -1 Torr is opened, a capacitance of 0.2μF is connected to the ground on the load side and a voltage of 6.9/√3≒4kV is applied, for example, and a discharge occurs between the electrodes. did. When this was captured by the antenna 16 and inputted to the detector 18, the signal from the amplifier had an amplitude of 0.6V when the gain was 10,000.
第6図は真空しや断器1が閉極状態であるとき
の本発明の第2実施例を示し、第7図は真空しや
断器1の閉極状態における等価回路である。この
第2実施例においてはループ状のアンテナ16a
を用い、このアンテナ16aを真空しや断器1の
近傍たとえば1mの位置に配設するものである。
アンテナ16aのループ部の径は10cmその直線部
の長さは5cmである。 FIG. 6 shows a second embodiment of the present invention when the vacuum shield breaker 1 is in the closed state, and FIG. 7 is an equivalent circuit of the vacuum shield breaker 1 in the closed state. In this second embodiment, a loop-shaped antenna 16a
The antenna 16a is placed near the vacuum shield breaker 1, for example, at a distance of 1 m.
The diameter of the loop part of the antenna 16a is 10 cm, and the length of the straight part is 5 cm.
上記第2実施例の真空度監視装置によれば、固
定リード5、可動リード7、固定電極8および可
動電極9と、浮遊電位である中間シールド10間
で真空度劣化時に放電が行なわれる。この場合、
リード棒および電極と中間シールド間の固有静電
容量は、開極時の電極間の見掛け上の静電容量に
比べて小さいためか、中間シールド10と大地間
の静電容量35が小さいため放電エネルギーも小
さく信号としても小さくなる。この場合、前述し
たように、例えば1m離れた位置にある真空度
10-1Torr程度の6.9kV/√3=4kVの電圧印加を
すると放電した。これをアンテナ16aで捕え検
出器に入力すると増幅器からの信号はゲインが
10000のとき0.3Vの振れ幅となつた。 According to the vacuum level monitoring device of the second embodiment, discharge occurs between the fixed lead 5, the movable lead 7, the fixed electrode 8, the movable electrode 9, and the intermediate shield 10 which is at a floating potential when the vacuum level deteriorates. in this case,
Discharge occurs probably because the specific capacitance between the lead rod and electrode and the intermediate shield is smaller than the apparent capacitance between the electrodes when they are open, or because the capacitance 35 between the intermediate shield 10 and the ground is small. The energy is small and the signal is also small. In this case, as mentioned above, for example, the degree of vacuum at a position 1 m away.
When a voltage of 6.9kV/√3=4kV of about 10 -1 Torr was applied, a discharge occurred. When this is captured by the antenna 16a and input to the detector, the signal from the amplifier has a gain
When it was 10000, the amplitude was 0.3V.
第8図は本発明の第3実施例を示し、41は後
述する真空しや断器が収納されたタンクで、その
内部には絶縁油,SF6などの絶縁媒体が注入され
ている。タンク41は鉄板あるいはステンレス鋼
板等の金属板によつて形成されている。42,4
2はブツシング、43,43は真空しや断器の可
動,固定電極に接続された外部接続導体、44は
タンク41を載置するための台枠である。 FIG. 8 shows a third embodiment of the present invention. Reference numeral 41 denotes a tank in which a vacuum shield and disconnector, which will be described later, is housed, and an insulating medium such as insulating oil or SF 6 is poured into the tank. The tank 41 is formed of a metal plate such as an iron plate or a stainless steel plate. 42,4
2 is a bushing; 43, 43 are external connection conductors connected to the movable and fixed electrodes of the vacuum shield breaker; and 44 is a frame on which the tank 41 is placed.
外部接続導体43,43の近傍には受信用アン
テナ16aが配設され、このアンテナ16aには
接続線17を介して検出器18が接続される。長
さが30cm,断面積が1.25mm2のビニール被覆銅線ケ
ーブルをアンテナ16aに使用したとき、ブツシ
ングから1m離れた位置にアンテナ16aを置く。
第9図は絶縁油又は絶縁ガス槽45中に真空しや
断器1と槽45間に接続したコンデンサ46を収
納している。前記コンデンサ46は0.25μFの静電
容量を有し、この容量は6.9kV級でリード線の1
Kmに相当する分の静電容量である。前記真空しや
断器1の真空度が0.3Torrであるとき電極を開
き、外部接続導体43,43間に例えば6.9kV/
√3=4kVの電圧を印加すると電極間にて放電
し、ブツシング47を通して外部接続導体43,
43に放電時に発生する信号が伝達される。長さ
が30cm、断面積が1.25mm2のビニール被覆銅線ケー
ブルをアンテナ16に使用したとき、固定側導体
のブツシング47から1m離れた位置にアンテナ
16を置き、前記信号をアンテナ16で受信し、
検出器18により増幅し、真空度劣化の警報,表
示を行う。 A reception antenna 16a is arranged near the external connection conductors 43, 43, and a detector 18 is connected to this antenna 16a via a connection line 17. When a vinyl-coated copper cable with a length of 30 cm and a cross-sectional area of 1.25 mm 2 is used as the antenna 16a, the antenna 16a is placed 1 m away from the bushing.
In FIG. 9, a capacitor 46 connected between the vacuum shield breaker 1 and the tank 45 is housed in an insulating oil or gas tank 45. The capacitor 46 has a capacitance of 0.25 μF, and this capacitance is 6.9 kV class and is connected to one of the lead wires.
This is the capacitance equivalent to Km. When the vacuum degree of the vacuum shield breaker 1 is 0.3 Torr, the electrodes are opened and a voltage of 6.9 kV/for example is applied between the external connection conductors 43 and 43.
When a voltage of √3=4kV is applied, a discharge occurs between the electrodes, and the external connection conductor 43,
A signal generated during discharge is transmitted to 43. When a vinyl-coated copper cable with a length of 30 cm and a cross-sectional area of 1.25 mm 2 is used as the antenna 16, the antenna 16 is placed 1 m away from the bushing 47 of the fixed conductor, and the signal is received by the antenna 16. ,
It is amplified by the detector 18, and an alarm and display of deterioration of the degree of vacuum are performed.
増幅信号は上記の電圧で利得10000にて0.4Vと
なる。 The amplified signal becomes 0.4V at the above voltage and a gain of 10000.
閉極時は電極およびリードと浮遊電位である中
間シールドとの間にて放電するが、外部へは開極
時と異なりブツシング47と外部接続導体43,
43を通して微弱な信号が空中に出る。このた
め、閉極時の真空バルブの真空度の良否は、真空
しや断器1の浮遊中間シールドとタンク壁(アー
ス)間をコンデンサ46で結合することにより、
測定可能な信号が開極時と同様に出るので真空度
の良否の判定ができる。 When the contact is closed, a discharge occurs between the electrode and the lead and the floating potential intermediate shield, but unlike when the contact is opened, the bushing 47 and the external connection conductor 43 are discharged to the outside.
A weak signal goes out into the air through 43. Therefore, the degree of vacuum of the vacuum valve during closing can be checked by connecting the floating intermediate shield of the vacuum shield breaker 1 and the tank wall (earth) with the capacitor 46.
Since a measurable signal is output in the same way as when the electrodes are opened, it is possible to judge whether the degree of vacuum is good or bad.
第10図および第11図はそれぞれ本発明の更
に他の実施例を示すもので、第10図の真空度監
視装置においては、全面が鉄板あるいはステンレ
ス鋼板等の金属板で覆われた縮小型開閉装置48
は真空しや断器(図示省略)を内蔵している。こ
の開閉装置48の外部にはブツシング49を通し
て外部接続導体43が突出している。これらのブ
ツシング49あるいは外部接続導体43の近傍に
はアンテナ16が配置されている。また、第11
図の真空度監視装置においては、変電装置48の
3相スペーサ50の近傍にアンテナ16および検
出器18を配置したものである。第10図および
第11図の実施例においても前述した実施例と同
様な作用,効果が得られる。 FIGS. 10 and 11 respectively show still other embodiments of the present invention. In the vacuum level monitoring device shown in FIG. device 48
has a built-in vacuum shield and disconnector (not shown). An external connection conductor 43 protrudes from the outside of this opening/closing device 48 through a bushing 49 . An antenna 16 is arranged near these bushings 49 or external connection conductors 43. Also, the 11th
In the vacuum monitoring device shown in the figure, an antenna 16 and a detector 18 are arranged near a three-phase spacer 50 of a power substation 48. The embodiments shown in FIGS. 10 and 11 also provide the same functions and effects as the embodiments described above.
従来、タンク型真空しや断器内にある真空バル
ブの真空度の良否は、油槽あるいはガス槽内の絶
縁油あるいは絶縁性ガスを抜き取り、その上で真
空バルブの電極間距離を耐圧試験用に調節して電
圧を印加し、耐電圧法により調べていた。このた
め非常に手間がかかるとともに、元に戻す際の人
為的な誤りも生じていたが、実施例によれば何ら
油槽,ガス槽をいじることなく、真空しや断器を
開極し、真空度劣化時パツシエンの法則に影響さ
れる前駆現象により電極間が放電するとき又は閉
極時には固定リード、固定電極、可動電極および
可動リードとシールド間が放電するときプツシン
グおよび印加線から出る放電信号を受信アンテナ
で受信し、このアンテナにより受信された信号を
電気的に処理して真空度劣化を検出することがで
きる。このため、真空度劣化の検出に際して真空
しや断器を回路から取外す必要がないとともに真
空しや断器の構造を変えたり高電圧の別電源を設
けたりする必要がなく、簡単かつ安価に真空度劣
化を正確に検出することができる。 Conventionally, the quality of the vacuum of the vacuum valve in a tank-type vacuum chamber or disconnector was determined by draining the insulating oil or insulating gas from the oil tank or gas tank, and then measuring the distance between the electrodes of the vacuum valve for a pressure test. The voltage was adjusted and tested using the withstand voltage method. This was extremely time-consuming and caused human error when restoring the original state, but according to the example, the vacuum chamber and disconnector were opened without any manipulation of the oil tank or gas tank, and the vacuum When there is a discharge between the electrodes due to a precursor phenomenon influenced by Patsien's law, or when the fixed lead, fixed electrode, movable electrode, or between the movable lead and the shield are discharged when the contact is closed, the discharge signal output from the pushing and application wires is It is possible to detect vacuum deterioration by receiving a signal with a receiving antenna and electrically processing the signal received by this antenna. Therefore, when detecting vacuum deterioration, there is no need to remove the vacuum shield or disconnector from the circuit, there is no need to change the structure of the vacuum shield or disconnector, or to install a separate high-voltage power supply. degree deterioration can be detected accurately.
上述の各実施例における真空度監視装置によれ
ば、既に使用されている真空しや断器に適用でき
るものであり、完全にアースシールドされている
ものも含む、ほとんどの機種に適用できるととも
に、活線状態で真空度劣化を検知できる。また、
検出部の電源としては商用電源又は電池を用いて
もよく、コンパクトとなり携帯に便利である。な
お、真空度劣化検出感度は放電ギヤツプが大のほ
うが高真空でもパツシエンの法則に影響される前
駆現象により放電々圧が低下するので検出可能と
なる又真空度劣化の圧力の値はほぼ10-3Torr台
から100Torr台である。 According to the vacuum level monitoring device in each of the above-mentioned embodiments, it can be applied to vacuum shields and disconnectors that are already in use, and can be applied to most models, including those that are completely earth-shielded. Deterioration of vacuum level can be detected in live line condition. Also,
A commercial power source or a battery may be used as a power source for the detection unit, which is compact and convenient to carry. In addition, the detection sensitivity of vacuum deterioration becomes more detectable when the discharge gap is large because the discharge pressure decreases due to a precursor phenomenon influenced by Patsien's law even in high vacuum, and the pressure value of vacuum deterioration is approximately 10 - It ranges from 3 Torr to 100 Torr.
以上のように本発明においては、真空しや断器
の外部に放電時に発生する2〜20kHzの高周波を
含む電磁波信号を受信するアンテナとバンドパス
フイルターを備えた検出器を設けており、このた
め真空しや断器は真空度劣化時に内部で放電を生
じ、このアンテナにより受信された信号を電気的
に処理して真空度劣化を検出することができるば
かりでなく、外部の電気的ノイズに影響されず感
度よく検出できる。更に真空度劣化の検出に際し
て真空しや断器を回路から取外す必要がないとと
もに真空しや断器の構造を変えたり高電圧の別電
源を設けたりする必要がなく、簡単かつ安価に真
空度劣化を正確に検出することができる。 As described above, in the present invention, a detector equipped with an antenna and a bandpass filter for receiving electromagnetic wave signals including high frequencies of 2 to 20 kHz generated during discharge is provided outside the vacuum shield and disconnector. Vacuum shield disconnectors generate internal discharge when the vacuum level deteriorates, and the signals received by this antenna can be electrically processed to detect the vacuum level deterioration, as well as being able to detect external electrical noise. It can be detected with high sensitivity. Furthermore, when detecting vacuum deterioration, there is no need to remove the vacuum shield or disconnector from the circuit, and there is no need to change the structure of the vacuum shield or disconnector or install a separate high-voltage power supply, making it easy and inexpensive to detect vacuum deterioration. can be detected accurately.
第1図は本発明の第1の実施例に係る真空度監
視装置を備えた真空しや断器の縦断正面図、第2
図Aは検出部の詳細を示すブロツク線図、第2図
Bは同上Aの出力図、第3図は第1の実施例にお
ける真空しや断器のしや断状態における等価回路
図、第4図A,Bおよび第5図A,Bは第1の実
施例における真空しや断器の動作波形図、第6図
は本発明の第2の実施例に係る真空度監視装置を
備えた真空しや断器の縦断正面図、第7図はその
等価回路、第8図は本発明の第3の実施例に係る
真空しや断器の真空度劣化検出装置を備えたタン
ク型しや断器の正面図、第9図は実験的に用いら
れた真空しや断器の縦断正面図、第10図および
第11図はそれぞれ本発明の他の実施例を示す真
空しや断器の真空度監視装置の正面図である。
1……真空しや断器、16,16a……アンテ
ナ、18……検出器、19……増幅器、20……
判定部。
FIG. 1 is a longitudinal sectional front view of a vacuum shield breaker equipped with a vacuum level monitoring device according to a first embodiment of the present invention;
Figure A is a block diagram showing the details of the detection section, Figure 2B is an output diagram of the same as above A, Figure 3 is an equivalent circuit diagram of the vacuum shield disconnector in the shielded state in the first embodiment, 4A, B and 5A, B are operation waveform diagrams of the vacuum shield breaker in the first embodiment, and FIG. 6 is a vacuum level monitoring device according to the second embodiment of the present invention. FIG. 7 is a longitudinal sectional front view of a vacuum shield disconnector, FIG. 7 is an equivalent circuit thereof, and FIG. 8 is a tank-type shield equipped with a vacuum degree deterioration detection device for a vacuum shield disconnector according to a third embodiment of the present invention. FIG. 9 is a front view of a vacuum sheath breaker used experimentally, and FIGS. 10 and 11 are views of a vacuum sheath breaker showing other embodiments of the present invention. FIG. 3 is a front view of the vacuum level monitoring device. 1... Vacuum shield disconnector, 16, 16a... Antenna, 18... Detector, 19... Amplifier, 20...
Judgment department.
Claims (1)
る真空しや断器において、真空しや断器の外部近
傍に設けられ、前記内部放電により生じる電磁波
信号を受信するアンテナと、該アンテナに電気的
に接続され、2kHzから20kHzの周波数成分のみを
通過させるバンドパスフイルタを備えた検出器か
らなることを特徴とする真空しや断器の真空度監
視装置。1. In a vacuum shield disconnector that generates an internal discharge when the degree of internal vacuum deteriorates, an antenna is installed near the outside of the vacuum shield disconnector and receives an electromagnetic wave signal generated by the internal discharge, and an electric wire is connected to the antenna. A vacuum degree monitoring device for a vacuum shield and disconnector, characterized by comprising a detector connected to the detector and equipped with a bandpass filter that passes only frequency components from 2kHz to 20kHz.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1267482A JPS58129338A (en) | 1982-01-29 | 1982-01-29 | Monitoring device for degree of vacuum of vacuum circuit breaker |
| EP82305761A EP0079181B1 (en) | 1981-10-30 | 1982-10-29 | Vacuum monitor for vacuum interrupter and use of the vacuum monitor |
| DE8282305761T DE3270153D1 (en) | 1981-10-30 | 1982-10-29 | Vacuum monitor for vacuum interrupter and use of the vacuum monitor |
| US06/437,678 US4547769A (en) | 1981-10-30 | 1982-10-29 | Vacuum monitor device and method for vacuum interrupter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1267482A JPS58129338A (en) | 1982-01-29 | 1982-01-29 | Monitoring device for degree of vacuum of vacuum circuit breaker |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58129338A JPS58129338A (en) | 1983-08-02 |
| JPS645648B2 true JPS645648B2 (en) | 1989-01-31 |
Family
ID=11811915
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1267482A Granted JPS58129338A (en) | 1981-10-30 | 1982-01-29 | Monitoring device for degree of vacuum of vacuum circuit breaker |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58129338A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN106840509A (en) * | 2016-12-29 | 2017-06-13 | 河南平高电气股份有限公司 | Vacuity of Vacuum Circuit Breakers on-line monitoring system based on superfrequency Cleaning Principle |
| CN114062919B (en) * | 2021-11-18 | 2022-08-02 | 广东电网有限责任公司广州供电局 | Rupture monitoring method, device, system and readable storage medium for vacuum interrupter |
-
1982
- 1982-01-29 JP JP1267482A patent/JPS58129338A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58129338A (en) | 1983-08-02 |
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