JPS6345052B2 - - Google Patents
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- Publication number
- JPS6345052B2 JPS6345052B2 JP13261680A JP13261680A JPS6345052B2 JP S6345052 B2 JPS6345052 B2 JP S6345052B2 JP 13261680 A JP13261680 A JP 13261680A JP 13261680 A JP13261680 A JP 13261680A JP S6345052 B2 JPS6345052 B2 JP S6345052B2
- Authority
- JP
- Japan
- Prior art keywords
- vacuum
- voltage
- light
- degree
- electro
- 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
- 239000003990 capacitor Substances 0.000 claims description 25
- 230000000694 effects Effects 0.000 claims description 12
- 238000012806 monitoring device Methods 0.000 claims description 12
- 230000010287 polarization Effects 0.000 claims description 4
- 238000012544 monitoring process Methods 0.000 description 15
- 238000010586 diagram Methods 0.000 description 12
- 238000001514 detection method Methods 0.000 description 11
- 230000007423 decrease Effects 0.000 description 7
- 239000013307 optical fiber Substances 0.000 description 6
- 239000004020 conductor Substances 0.000 description 4
- 239000002184 metal Substances 0.000 description 4
- 230000006866 deterioration Effects 0.000 description 3
- 230000005684 electric field Effects 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- NMFHJNAPXOMSRX-PUPDPRJKSA-N [(1r)-3-(3,4-dimethoxyphenyl)-1-[3-(2-morpholin-4-ylethoxy)phenyl]propyl] (2s)-1-[(2s)-2-(3,4,5-trimethoxyphenyl)butanoyl]piperidine-2-carboxylate Chemical compound C([C@@H](OC(=O)[C@@H]1CCCCN1C(=O)[C@@H](CC)C=1C=C(OC)C(OC)=C(OC)C=1)C=1C=C(OCCN2CCOCC2)C=CC=1)CC1=CC=C(OC)C(OC)=C1 NMFHJNAPXOMSRX-PUPDPRJKSA-N 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000012886 linear function Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 238000012887 quadratic function Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 238000000638 solvent extraction Methods 0.000 description 1
Classifications
-
- 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
- Measuring Fluid Pressure (AREA)
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
Description
【発明の詳細な説明】
本発明は、真空インターラプタに並列に分担電
圧均一化コンデンサを具える真空開閉器の真空度
監視装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum level monitoring device for a vacuum switch, which includes a shared voltage equalizing capacitor in parallel with a vacuum interrupter.
真空しや断器などの真空開閉器にあつては、そ
の真空度の低下はしや断能力劣化など開閉器の能
力に大きく影響し、適用設備の信頼性向上には真
空度監視が望まれる。 In the case of vacuum switches such as vacuum switches and disconnectors, a decrease in the degree of vacuum can greatly affect the performance of the switch, such as a decrease in the degree of vacuum or a deterioration in the disconnection ability, so monitoring the degree of vacuum is desirable to improve the reliability of the equipment in which it is applied. .
真空度監視の従来技術としては、真空インター
ラプタ内に開閉電極とは別個に監視用の一対の対
向電極を用意しておき、該一対の対向電極間の放
電電圧を計測するものがあるが、これには真空イ
ンターラプタそのものを特別に設計する必要があ
るし、対向電極間に電圧印加する高圧電源を用意
するなど監視装置としては大型、高価なものにな
る欠点があつた。また、監視装置と開閉電極間に
充分な絶縁を得るのが難しかつた。 As a conventional technique for monitoring the degree of vacuum, there is a method in which a pair of opposing electrodes for monitoring is prepared separately from the opening/closing electrode in a vacuum interrupter, and the discharge voltage between the pair of opposing electrodes is measured. This requires a special design of the vacuum interrupter itself, and it also requires a high-voltage power source to apply voltage between opposing electrodes, making the monitoring device large and expensive. Also, it was difficult to obtain sufficient insulation between the monitoring device and the switching electrode.
上記問題点を解消した装置として、真空インタ
ーラプタの真空度低下をその周囲の電界変化とし
て捕え、電界の変化をポツケルス素子による屈折
率変化とし、この屈折率を検光子と受光素子で検
出するものを本願出願人は既に提案している(特
願昭55−37098号)。 A device that solves the above problems is one that captures the decrease in the degree of vacuum in the vacuum interrupter as a change in the electric field around it, converts the change in the electric field into a change in refractive index using a Pockels element, and detects this refractive index with an analyzer and a light receiving element. The applicant has already proposed this (Japanese Patent Application No. 37098/1983).
本発明は、真空インターラプタに並列に分担電
圧均一化コンデンサを具える真空開閉器において
は該コンデンサに印加される電圧が真空インター
ラプタの真空度によつて変化することに着目し、
該コンデンサをポツケルス素子やカー素子などの
電気光学効果素子への電界印加手段とすることに
より、真空インターラプタと電気光学効果素子の
結合を容易にすると共に確実な真空度監視を可能
とし、さらに複数の真空開閉器を並列、直列接続
する設備に適用して監視装置の効率的な構成にで
きるようにした真空度監視装置を提供することを
目的とする。 The present invention focuses on the fact that in a vacuum switch including a shared voltage equalizing capacitor in parallel with a vacuum interrupter, the voltage applied to the capacitor changes depending on the degree of vacuum of the vacuum interrupter,
By using the capacitor as a means for applying an electric field to an electro-optic effect element such as a Pockels element or a Kerr element, it is possible to easily connect the vacuum interrupter and the electro-optic effect element, and also to enable reliable monitoring of the degree of vacuum. It is an object of the present invention to provide a vacuum level monitoring device that can be applied to equipment in which vacuum switches of 1 to 6 are connected in parallel or in series to provide an efficient configuration of the monitoring device.
以下、図面を参照して本発明の原理的説明を及
び実施例を説明する。 Hereinafter, the principles and embodiments of the present invention will be explained with reference to the drawings.
第1図は、真空インターラプタの周囲にアース
接地された金属ケースを持つタンク型真空しや断
器の要部側断面図を示す。ガラス筒などの絶縁円
筒1はその両端板2,3によつて真空容器が構成
され、一方の端板2を貫通して容器内に電極を持
つ固定リード4が設けられ、他方の端板3にはベ
ローズ5を容器内外仕切手段として該ベローズ5
を介して容器内に電極を持つ可動リード6が設け
られる。また、端板2,3の表面にはリード4,
6に夫々電気接続された導体7,8が設けられ、
該導体7,8間には容器外部に分担電圧均一化コ
ンデンサ91〜92oが直列接続で設けられる。こ
の真空インターラプタの最外側には該インターラ
プタを絶縁性ガスを含んで収納する金属容器10
がアース接地して設けられる。また、コンデンサ
91〜92oの中間接続点は中間シールド11に電
気接続され、その点の電位がほぼ50%にされる
し、真空容器内の電位分布も均等にされる。 FIG. 1 shows a sectional side view of a main part of a tank-type vacuum interrupter having a metal case that is grounded around a vacuum interrupter. An insulating cylinder 1 such as a glass tube has both end plates 2 and 3 forming a vacuum container, and a fixed lead 4 having an electrode is provided inside the container by penetrating one end plate 2. The bellows 5 is used as a means for partitioning the inside and outside of the container.
A movable lead 6 having an electrode is provided inside the container via the container. Also, on the surfaces of the end plates 2 and 3, leads 4,
6 are provided with conductors 7 and 8 electrically connected to each other,
Between the conductors 7 and 8, shared voltage equalizing capacitors 9 1 to 9 2o are connected in series outside the container. On the outermost side of this vacuum interrupter is a metal container 10 containing an insulating gas and housing the interrupter.
is connected to earth. Further, the intermediate connection points of the capacitors 9 1 to 9 2o are electrically connected to the intermediate shield 11, and the potential at that point is set to approximately 50%, and the potential distribution within the vacuum container is also made uniform.
こうした構成の真空しや断器において、固定リ
ード4に交流電源12を接続し、可動リード6に
負荷13を接続した運転状態で、可動リード6を
固定リード4に接触させた閉極時の等価回路は第
2図に示すものになる。第2図中、R1は絶縁円
筒1の抵抗分、R2はリード4,6とシールド1
1間の抵抗、Cpはリード4,6とシールド11間
の浮遊容量、C1はコンデンサ91〜92oにおける
上半分と下半分の総容量、C2はシールド11及
びコンデンサ91〜92oと金属容器10間の浮遊
容量である。 In a vacuum shield/disconnector having such a configuration, the equivalent of closing when the movable lead 6 is brought into contact with the fixed lead 4 in an operating state in which the AC power supply 12 is connected to the fixed lead 4 and the load 13 is connected to the movable lead 6. The circuit will be as shown in FIG. In Figure 2, R1 is the resistance of the insulating cylinder 1, and R2 is the resistance of the leads 4, 6 and the shield 1.
C p is the stray capacitance between the leads 4, 6 and the shield 11, C 1 is the total capacitance of the upper and lower halves of the capacitors 9 1 to 9 2o , C 2 is the resistance between the shield 11 and the capacitors 9 1 to 9 2o and the floating capacitance between the metal container 10.
この等価回路からも明らかなように、真空容器
1の真空度が良好な場合、真空インターラプタで
の各部電圧は以下のようになる。 As is clear from this equivalent circuit, when the degree of vacuum in the vacuum vessel 1 is good, the voltages at various parts of the vacuum interrupter are as follows.
VAB=C2/C0+C1+C2V ……(1)
VAE=C0+C1/C0+C1+C2V ……(2)
EC=EAB/n ……(3)
但し、VABは第2図中のA点とB点間電圧、
VAEはA点とアースE間電圧、Vは電源12の電
圧である。この(1)〜(3)式において、通常のインタ
ラプタはC0≪C1、C2≪C1であるから、VAB<VAE
となる。そして、真空度が低下すると、VABは零
に向かつて下り、VAEはVに向かつて上昇し、コ
ンデンサ91〜92oの各個の電圧ECは零に向かつ
て下る。この関係を第3図に横軸に真空容器内圧
力を、縦軸にEAE・EAB・ECを取つて示す。圧力
P1以下は真空度正常とされる値を、P2以上は真
空度劣化とされる値を示し、P1とP2間に電圧
EAE・EAB・ECに変化が見られる。なお、可動リ
ード6を固定リード4から引外した開極時の等価
回路は抵抗R2と浮遊容量C0が夫々リード6及び
4に分割され、リード6と4間に抵抗と浮遊容量
の並列回路が介在する状態になり、この等価回路
になる開極時の電圧EAE、EAB、ECもレベルの変
化はあるが真空度の変化によつて閉極時と同様の
現象を呈する。 V AB =C 2 /C 0 +C 1 +C 2 V ......(1) V AE =C 0 +C 1 /C 0 +C 1 +C 2 V ......(2) E C =E AB /n ...(3) However, V AB is the voltage between point A and point B in Figure 2,
VAE is the voltage between point A and earth E, and V is the voltage of the power supply 12. In these equations (1) to (3), since the normal interrupter is C 0 ≪C 1 and C 2 ≪C 1 , V AB <V AE
becomes. Then, when the degree of vacuum decreases, V AB decreases toward zero, V AE increases toward V, and the voltage E C of each of the capacitors 9 1 to 9 2o decreases toward zero. This relationship is shown in Figure 3, with the vacuum vessel internal pressure on the horizontal axis and E AE , E AB , and E C on the vertical axis. pressure
P 1 or less indicates a value that is considered normal vacuum, P 2 or more indicates a degraded vacuum, and there is no voltage between P 1 and P 2 .
Changes are seen in E AE , E AB , and E C. The equivalent circuit when the movable lead 6 is disconnected from the fixed lead 4 is that the resistance R 2 and the stray capacitance C 0 are divided into the leads 6 and 4, respectively, and the resistance and stray capacitance are connected in parallel between the leads 6 and 4. A circuit is interposed, and the voltages E AE , E AB , and E C at the time of opening, which become this equivalent circuit, exhibit a phenomenon similar to that at the time of closing due to changes in the degree of vacuum, although there are changes in level.
従つて、これら電圧EAB又はEAE又はECを監視
することで真空度の良否を判定でき、本発明にお
いては分担電圧均一化コンデンサ電圧ECの監視
による真空度良否を判定する。この電圧ECの監
視は他の電圧EAEもしくはEABの監視に比してコン
デンサ単体の両端電圧を検出することから検出素
子の取付け、取外しを容易にし、既設の真空開閉
器への監視装置設置及び保守・点検を容易にす
る。 Therefore, the degree of vacuum can be determined by monitoring these voltages E AB , E AE , or E C , and in the present invention, the degree of vacuum is determined by monitoring the shared voltage equalization capacitor voltage E C. Compared to monitoring other voltages E AE or E AB , monitoring of this voltage E C detects the voltage across a single capacitor, making it easier to install and remove the detection element, and it can be used as a monitoring device for existing vacuum switches. Facilitates installation, maintenance and inspection.
第4図は本発明による監視装置の基本的ブロツ
ク図を示す。分担電圧均一化コンデンサ電圧EC
はポツケルス素子やカー素子などの電気光学効果
素子14に印加し、この電気光学効果素子14は
偏光子15と検光子16間に配置された構成の真
空度検出ヘツド17としてコンデンサに一体的に
取付け、偏光子15には光源18から該検出ヘツ
ド17位置まで光フアイバーの光伝送路を経て光
入射をなし、該偏光子15で直線偏光された光を
電気光学効果素子14を通すことで電圧ECに一
次関数又は二次関数関係で屈折させ、この光を検
光子16を通して該検光子の偏光方向成分を光−
電気変換素子の受光部19で検出し、この検出電
気信号レベルで比較器等の判定部20で判定する
ことで真空度良否の表示さらには警報信号を得
る。 FIG. 4 shows a basic block diagram of a monitoring device according to the invention. Shared voltage equalization capacitor voltage E C
is applied to an electro-optic effect element 14 such as a Pockels element or a Kerr element, and this electro-optic effect element 14 is integrally attached to a capacitor as a vacuum degree detection head 17 arranged between a polarizer 15 and an analyzer 16. , light enters the polarizer 15 from the light source 18 to the detection head 17 position via an optical fiber transmission path, and the light linearly polarized by the polarizer 15 passes through the electro-optic effect element 14 to generate a voltage E. C is refracted in a linear or quadratic function relationship, and this light is passed through an analyzer 16 to determine the polarization direction component of the analyzer.
It is detected by the light receiving section 19 of the electrical conversion element, and a judgment section 20 such as a comparator makes a judgment based on the detected electric signal level, thereby obtaining an indication of whether the degree of vacuum is good or not, as well as an alarm signal.
第4図における真空度検出ヘツド17を真空イ
ンターラプタに取付ける具体的構造は第5図に示
す。第5図において、分担電圧均一化コンデンサ
91〜92oのうちの1つである最下部のコンデン
サ92oの両端から引出した導体21,21を検出
ヘツド17の電圧印加端子に接続及びその支持部
材とし、検出ヘツド17の光入力には地上側光源
18から光フアイバー22で良好なる絶縁性を持
つて送り、検出ヘツド17の光出力は光フアイバ
ー23を通して地上側受光部19さらに判定部2
0に送る。なお、検出ヘツド17の容量はコンデ
ンサ92oのそれに比して充分に小さく該コンデン
サ92oの容量精度に影響を与えるものでないし、
また検出ヘツド17の耐圧が低い場合には該ヘツ
ド内に分圧用コンデンサを直列接続する構成は容
易に実現される。 A concrete structure for attaching the vacuum detecting head 17 shown in FIG. 4 to the vacuum interrupter is shown in FIG. In FIG. 5, conductors 21, 21 drawn out from both ends of the lowest capacitor 92o, which is one of the shared voltage equalizing capacitors 91 to 92o , are connected to the voltage application terminal of the detection head 17 and supported. The light input to the detection head 17 is sent from the ground-side light source 18 through an optical fiber 22 with good insulation, and the light output from the detection head 17 is transmitted through the optical fiber 23 to the ground-side light receiving section 19 and then to the judgment section 2.
Send to 0. Note that the capacitance of the detection head 17 is sufficiently smaller than that of the capacitor 92o and does not affect the capacitance accuracy of the capacitor 92o .
Further, when the detection head 17 has a low breakdown voltage, a configuration in which a voltage dividing capacitor is connected in series within the head can be easily realized.
実施例においては、1本の真空インターラプタ
に適用する場合を示したが、本発明はこれに限定
されるものでなく、1相2本直列の場合や3相2
本直列の場合に適用して同等の作用効果を得るこ
とができるし、それらを一括した監視装置の実現
も可能である。 In the embodiment, a case where the vacuum interrupter is applied to one vacuum interrupter is shown, but the present invention is not limited to this.
The same effects can be obtained by applying this method in series, and it is also possible to realize a monitoring device that integrates them all together.
第6図は1相2本直列の場合の等価回路を示
し、その真空度良好なるときの等価回路は第7図
に示され、第7図中のC3=C0+C1、C4=C1/2
に相当し、第2図の場合と同様に分担電圧均一化
コンデンサの電圧監視により2本の真空インター
ラプタを一括した真空度監視ができる。この一括
監視の装置構成は第8図に示し、2本の真空イン
ターラプタの夫々の1つの分担電圧均一化コンデ
ンサに電気光学効果素子14A,14Bを並列に
設け、両素子14A,14Bは互いに偏光面を直
角にしそのうちの14Aは受光側に偏光子15A
を、出力側に偏光子15Bを設け、偏光子15B
を出た光を素子14Bの受光偏光面として該素子
14Bの出力側に検光子16を設ける検出ヘツド
とし、両素子間の光伝送は光フアイバーを使用す
る。この構成において、何れか一方又は両方に真
空度劣化が生じると、検光子16を通す光の強さ
が低下しその判定出力を得ることができる。 Figure 6 shows an equivalent circuit in the case of one phase with two wires in series, and the equivalent circuit when the degree of vacuum is good is shown in Figure 7. In Figure 7, C 3 = C 0 + C 1 , C 4 = C 1/2
Similarly to the case of FIG. 2, the degree of vacuum of the two vacuum interrupters can be monitored at once by monitoring the voltage of the shared voltage equalizing capacitor. The device configuration for this collective monitoring is shown in FIG. 8, in which electro-optic effect elements 14A and 14B are provided in parallel to one shared voltage equalization capacitor of each of the two vacuum interrupters, and both elements 14A and 14B polarize each other. The planes are at right angles, and 14A of them are polarizers 15A on the receiving side.
, a polarizer 15B is provided on the output side, and the polarizer 15B is
The light emitted from the element 14B is used as a detection head with an analyzer 16 provided on the output side of the element 14B, and an optical fiber is used for optical transmission between the two elements. In this configuration, if deterioration of the degree of vacuum occurs in one or both of them, the intensity of light passing through the analyzer 16 decreases, and a determination output thereof can be obtained.
第9図は3相一括した真空度監視のための構造
図であり、第8図の場合と同様に偏光子15A〜
15Cと偏光面が交互に直角になる電気光学効果
素子14A〜14Cを交互に配置する光学系を構
成して3相の真空インターラプタの少なくとも1
本の真空度劣化でその検出をすることができる。 FIG. 9 is a structural diagram for monitoring the degree of vacuum in three phases at once, and as in the case of FIG.
At least one of the three-phase vacuum interrupters constitutes an optical system in which electro-optic effect elements 14A to 14C whose polarization planes are alternately perpendicular to 15C are arranged alternately.
This can be detected by the deterioration of the vacuum level of the book.
同様に、第10図に示すように、1相2本直列
の真空インターラプタを3相一括監視する構成に
できる。 Similarly, as shown in FIG. 10, two vacuum interrupters per phase can be configured to monitor three phases at once.
これら一括監視は第8図〜第10図からも明ら
かなように、受光部19光源18、判定部20を
1個用意して構成できるし、インターラプタ本数
当りの偏光子の使用個数も低減できる。 As is clear from FIGS. 8 to 10, this collective monitoring can be configured by preparing one light receiving section 19, one light source 18, and one determining section 20, and the number of polarizers used per number of interrupters can be reduced. .
以上のとおり、本発明による真空度監視装置
は、電圧分担均一化コンデンサを有する真空開閉
器に適用してその構造を変更することなく真空度
監視が容易にできる。また、複数本の真空開閉器
を持つ設備の監視にはその一括監視が容易にかつ
比較的低コストに実現できる。また、光フアイバ
ーによる大地と高圧部の絶縁を取ることができる
こと、検出ヘツドは電源を必要としない受動素子
でその信頼性も高いこと、真空インターラプタの
開極、閉極いずれの場合も監視ができること、及
び偏光度合による現象を利用した真空度検出のた
め電気ノイズ耐性に優れることなど、真空開閉器
への結合を容易にして確実な監視が可能となる。 As described above, the vacuum level monitoring device according to the present invention can be applied to a vacuum switch having a voltage sharing equalization capacitor to easily monitor the vacuum level without changing its structure. Furthermore, when monitoring equipment having a plurality of vacuum switches, collective monitoring can be easily realized at a relatively low cost. In addition, the high-voltage part can be insulated from the ground using optical fiber, the detection head is a passive element that does not require a power supply and is highly reliable, and the vacuum interrupter can be monitored whether it is open or closed. It also has excellent resistance to electrical noise because it detects the degree of vacuum using a phenomenon based on the degree of polarization, making it easy to connect to a vacuum switch and enable reliable monitoring.
なお、本発明はタンク型真空開閉器に限らず、
金属容器10に代る碍管を持つものさらには外囲
容器と真空インターラプタとの間の絶縁ガスに代
る固体絶縁物を充填した真空開閉器に適用して同
等の作用効果を得ることができる。 Note that the present invention is not limited to tank-type vacuum switches;
The same effect can be obtained by applying it to a vacuum switch that has an insulated tube instead of the metal container 10, or a vacuum switch filled with a solid insulator instead of an insulating gas between the envelope and the vacuum interrupter. .
第1図は電圧分担均一化コンデンサを有する真
空しや断器の概形図、第2図はその開極時の等価
回路図、第3図は第2図における真空度−電圧特
性図、第4図は本発明に係る監視装置ブロツク
図、第5図は本発明における要部取付構造図、第
6図は真空しや断器の2本直列接続における等価
回路図、第7図は第6図を変形した等価回路図、
第8図〜第10図は本発明の他の監視装置ブロツ
ク図である。
1……真空容器、91〜92o……電圧分担均一
化コンデンサ、14……電気光学効果素子、15
……偏光子、16……検光子、17……真空度検
出ヘツド、18……光源、19……受光部、20
……判定部、21……導体、22,23……光フ
アイバー。
Figure 1 is a schematic diagram of a vacuum shield breaker with a voltage sharing equalization capacitor, Figure 2 is an equivalent circuit diagram when it is open, Figure 3 is a vacuum degree-voltage characteristic diagram in Figure 2, and Figure 4 is a block diagram of a monitoring device according to the present invention, Figure 5 is a diagram of the main part mounting structure of the present invention, Figure 6 is an equivalent circuit diagram of two vacuum shield disconnectors connected in series, and Figure 7 is an equivalent circuit diagram of two vacuum shield disconnectors connected in series. Equivalent circuit diagram modified from the diagram,
8 to 10 are block diagrams of other monitoring devices according to the present invention. 1... Vacuum container, 9 1 to 9 2o ... Voltage sharing equalization capacitor, 14... Electro-optic effect element, 15
... Polarizer, 16 ... Analyzer, 17 ... Vacuum degree detection head, 18 ... Light source, 19 ... Light receiving section, 20
. . . Determination section, 21 . . . Conductor, 22, 23 . . . Optical fiber.
Claims (1)
シールドに中間接続点が電気接続される電圧分担
均一化のための複数の直列コンデンサを有する真
空開閉器において、前記コンデンサの1つのコン
デンサの両端電圧が屈折率制御電圧として印加さ
れる電気光学効果素子と、光源からの光を直線偏
光して前記電気光学効果素子に光入射させる偏光
子と、前記電気光学効果素子の屈折光出力から所
定の偏光方向成分の光を検出する検光子と、この
検出子の出力光を対応する電気信号に変換する受
光部と、この受光部の検出電気信号レベルが所定
値を越えたときに前記真空容器内の真空度劣化と
判定する判定部とを備えたことを特徴とする真空
開閉器の真空度監視装置。1. In a vacuum switch having a plurality of series capacitors for equalizing voltage sharing in which the switching electrodes are connected in parallel outside the vacuum vessel and the intermediate connection point is electrically connected to the intermediate shield, both ends of one of the capacitors an electro-optic effect element to which a voltage is applied as a refractive index control voltage; a polarizer that linearly polarizes light from a light source and makes it enter the electro-optic effect element; an analyzer that detects light with a polarization direction component; a light receiver that converts the output light of the detector into a corresponding electrical signal; A vacuum level monitoring device for a vacuum switch, comprising: a determination unit that determines that the vacuum level has deteriorated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13261680A JPS5757426A (en) | 1980-09-24 | 1980-09-24 | Vacuum degree monitor for vacuum switch |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13261680A JPS5757426A (en) | 1980-09-24 | 1980-09-24 | Vacuum degree monitor for vacuum switch |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5757426A JPS5757426A (en) | 1982-04-06 |
| JPS6345052B2 true JPS6345052B2 (en) | 1988-09-07 |
Family
ID=15085488
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13261680A Granted JPS5757426A (en) | 1980-09-24 | 1980-09-24 | Vacuum degree monitor for vacuum switch |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5757426A (en) |
-
1980
- 1980-09-24 JP JP13261680A patent/JPS5757426A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5757426A (en) | 1982-04-06 |
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