JPH0121573B2 - - Google Patents
Info
- Publication number
- JPH0121573B2 JPH0121573B2 JP5278881A JP5278881A JPH0121573B2 JP H0121573 B2 JPH0121573 B2 JP H0121573B2 JP 5278881 A JP5278881 A JP 5278881A JP 5278881 A JP5278881 A JP 5278881A JP H0121573 B2 JPH0121573 B2 JP H0121573B2
- Authority
- JP
- Japan
- Prior art keywords
- vacuum
- electric field
- light
- degree
- shield
- 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
- 230000005684 electric field Effects 0.000 claims description 47
- 238000001514 detection method Methods 0.000 claims description 28
- 230000010287 polarization Effects 0.000 claims description 16
- 238000012806 monitoring device Methods 0.000 claims description 9
- 239000007787 solid Substances 0.000 claims description 7
- 239000011810 insulating material Substances 0.000 claims description 2
- 230000003287 optical effect Effects 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 6
- 230000035945 sensitivity Effects 0.000 description 5
- 230000007423 decrease Effects 0.000 description 3
- 230000006866 deterioration Effects 0.000 description 3
- 238000009413 insulation Methods 0.000 description 3
- 238000012544 monitoring process Methods 0.000 description 3
- 239000013307 optical fiber Substances 0.000 description 3
- 239000013078 crystal Substances 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Measuring Fluid Pressure (AREA)
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
Description
【発明の詳細な説明】
本発明は真空しや断器などの真空開閉器の真空
度監視装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vacuum monitoring device for a vacuum switch such as a vacuum switch or disconnector.
一般に真空しや断器などの真空開閉器は内部の
真空度の良否によつて能力が大きく左右されるた
め真空度を監視することが必要となる。このため
従来においても種々の真空度監視装置が提案され
ているが、いずれも絶縁、大きさ、コストなどに
おいて問題があり、実用的でなかつた。 In general, the performance of vacuum switches such as vacuum switches and disconnectors is greatly affected by the quality of the internal vacuum, so it is necessary to monitor the vacuum. For this reason, various vacuum degree monitoring devices have been proposed in the past, but all of them have problems with insulation, size, cost, etc., and are not practical.
本発明は上記の従来の欠点を除去して、構成が
簡単小形で安価であるとともに絶縁上の問題もな
く、かつ真空度を常時高い信頼性で監視すること
ができるとともに設置が容易な真空開閉器の真空
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 conventional drawbacks, and has a simple, small, and inexpensive configuration, no problems with insulation, the ability to constantly monitor the degree of vacuum with high reliability, and a vacuum switch that is easy to install. The purpose of this invention is to provide a device for monitoring the degree of vacuum in a vessel.
以下本発明の実施例を図面とともに説明する。
まず、本発明の基本的な考え方を第1図A,B、
第2図および第3図A,Bによつて説明する。第
1図A,Bは夫々通電状態における真空しや断器
およびその等価回路を示し、1は固定電極、2は
可動電極、3は固定リード、4は可動リード、5
は絶縁筒、6,7は絶縁筒5の両端に封着された
端板で、固定リード3は端板6に取付けられ、可
動リード4はベローズ8を介して端板7に封着さ
れる。9は絶縁筒5の中間に取付けられたシール
ドである。又、10,11は夫々真空しや断器の
設置された回路の電源および負荷、12,13は
夫々固定電極1とシールド9間の抵抗および静電
容量、14,15は夫々可動電極2とシールド9
間の抵抗および静電容量、16a,16bは絶縁
筒5の抵抗、17はシールド9と大地間の静電容
量である。 Embodiments of the present invention will be described below with reference to the drawings.
First, the basic idea of the present invention is shown in FIGS. 1A and B.
This will be explained with reference to FIG. 2 and FIGS. 3A and 3B. Figures 1A and 1B show a vacuum shield breaker and its equivalent circuit in a energized state, where 1 is a fixed electrode, 2 is a movable electrode, 3 is a fixed lead, 4 is a movable lead, and 5 is a movable lead.
is an insulating tube, 6 and 7 are end plates sealed to both ends of the insulating tube 5, the fixed lead 3 is attached to the end plate 6, and the movable lead 4 is sealed to the end plate 7 via a bellows 8. . 9 is a shield attached to the middle of the insulating cylinder 5. Further, 10 and 11 are the power supply and load of the circuit in which the vacuum shield and circuit breaker are installed, 12 and 13 are the resistance and capacitance between the fixed electrode 1 and the shield 9, respectively, and 14 and 15 are the movable electrode 2 and the load, respectively. shield 9
16a and 16b are the resistances of the insulating tube 5, and 17 is the capacitance between the shield 9 and the ground.
上記した真空しや断器の内部は高真空に保たれ
ており、この真空度が劣化した場合に、静電容量
13,15はε0(真空誘電率)≒ε大気(大気中の
誘電率)であるから一定であるが抵抗12,14
は急激に小さくなる。このため、電極1,2とシ
ールド9間の電圧が小さくなり、真空しや断器の
各部での分担電圧に変化が生じる。例えば真空度
が良好な場合には電源10の電圧をV、固定電極
1とシールド9間の電圧をV1、可動電極2とシ
ールド9間の電圧をV2、シールド9と大地間の
電圧をV3としてV1=V2=V/2、V3=V−V1=V/2
となるが、真空度が劣化した場合にはV1=V2=
V/4、V3=V−V/4=3/4Vとなる(尚、これら
の
値は一例として示したもので真空しや断器の構造
や真空度によつて変化する。)。従つて、第2図に
示すようにシールド9の電圧V3は真空度によつ
て大きく変化し、シールド9付近の電界Eも大き
く変化する。 The interior of the above-mentioned vacuum shield and disconnector is maintained at a high vacuum, and when this degree of vacuum deteriorates, the capacitances 13 and 15 will change as follows: ε 0 (vacuum dielectric constant) ≒ ε atmosphere (atmospheric dielectric constant ), so the resistance is constant, but the resistance 12, 14
decreases rapidly. For this reason, the voltage between the electrodes 1, 2 and the shield 9 becomes small, and the voltages shared at each part of the vacuum shield and disconnector change. For example, when the degree of vacuum is good, the voltage of the power supply 10 is V, the voltage between the fixed electrode 1 and the shield 9 is V1 , the voltage between the movable electrode 2 and the shield 9 is V2, and the voltage between the shield 9 and the ground is V1. As V 3 , V 1 = V 2 = V/2, V 3 = V-V 1 = V/2, but if the degree of vacuum deteriorates, V 1 = V 2 =
V/4, V 3 =V-V/4=3/4V (These values are shown as an example and will vary depending on the structure of the vacuum chamber or disconnector and the degree of vacuum.) Therefore, as shown in FIG. 2, the voltage V 3 across the shield 9 varies greatly depending on the degree of vacuum, and the electric field E near the shield 9 also varies greatly.
又、第3図A,Bは夫々しや断状態における真
空しや断器およびその等価回路を示し、18,1
9は夫々電極1,2間の抵抗および静電容量を示
す。この場合も静電容量13,15,19は真空
度によつて変化しないが、抵抗12,14,18
は真空度によつて変化し、従つて真空度が劣化す
るとシールド9の電圧は上昇し、シールド9付近
の電界も大きくなる。このように真空しや断器に
おいては通電状態でもしや断状態でもシールド9
の電位が真空度によつて大きく変化し、シールド
9付近の電界も大きく変化する。従つて、シール
ド9の外部側の電界を監視することにより真空し
や断器の真空度を常時監視することができる。
又、これに伴つて絶縁筒5の外部側の電界を監視
することによつても真空度を監視することができ
る。 Moreover, FIGS. 3A and 3B show the vacuum shield disconnector and its equivalent circuit in the disconnected state, respectively, and 18 and 1
9 indicates the resistance and capacitance between electrodes 1 and 2, respectively. In this case as well, the capacitances 13, 15, 19 do not change depending on the degree of vacuum, but the resistances 12, 14, 18
varies depending on the degree of vacuum. Therefore, when the degree of vacuum deteriorates, the voltage across the shield 9 increases and the electric field near the shield 9 also increases. In this way, in a vacuum disconnector, the shield 9
The potential changes greatly depending on the degree of vacuum, and the electric field near the shield 9 also changes greatly. Therefore, by monitoring the electric field on the outside of the shield 9, it is possible to constantly monitor the degree of vacuum in the vacuum shield and the disconnector.
Additionally, the degree of vacuum can also be monitored by monitoring the electric field on the outside of the insulating cylinder 5.
又、第4図は本発明に係る真空度監視装置の基
本的構成を示し、20は偏光子、21は電界検知
部で、電界検知部21としてはポツケルス素子又
はカー素子を用いるが、この場合はポツケルス素
子として説明する。22は検光子、23は光源、
24は受光部である。その動作を説明すると、光
源23から発せられた光は偏光子20に送られ、
偏光子20により水平方向又は垂直方向に直線偏
光される。電界検知部21は例えば真空しや断器
のシールド9の外側部近傍に設けられており、該
位置での電界Eを加えられ(電界Eの方向はポツ
ケルス素子の結晶軸により定める。)、電界Eの大
きさに応じて偏光子20からの光の偏光面角度を
θだけ変化させる。電界検知部21を通過した光
は偏光面が偏光子20の偏光面と所定な関係にあ
る検光子22に加えられ、検光子22を通過した
光は光量に応じた電気信号を出す受光部に加えら
れる。第5図に示すように真空しや断器の真空度
が良好な場合にはシールド9の外部側近傍の電界
Eは小さく、真空度が劣化すると電界Eは大きく
なる。従つて、電界検知部21における光の偏光
面の変化角θは真空度が良好な場合には小さく、
真空度が不良になるとθは大きくなる。このた
め、検光子22の偏光面と偏光子20の偏光面が
直角な場合には真空度が不良になると検光子22
を通過する光量が多くなり、受光部24の出力A
は第5図の実線で示すように大きくなる。又、検
光子22と偏光子20の偏光面が平行な場合には
真空度が不良になると検光子22を通過する光量
が少くなり、受光部24の出力Aは第5図の点線
で示すように小さくなる。従つて、受光部24の
出力が急激に大きく又は小さくなつたことにより
真空度劣化を検知することができる。 Further, FIG. 4 shows the basic configuration of the vacuum level monitoring device according to the present invention, 20 is a polarizer, 21 is an electric field detection section, and as the electric field detection section 21, a Pockels element or a Kerr element is used. will be explained as a Pockels element. 22 is an analyzer, 23 is a light source,
24 is a light receiving section. To explain its operation, light emitted from the light source 23 is sent to the polarizer 20,
The polarizer 20 linearly polarizes the light in the horizontal or vertical direction. The electric field detection unit 21 is provided, for example, near the outer side of the shield 9 of a vacuum shield breaker, and is applied with an electric field E at that position (the direction of the electric field E is determined by the crystal axis of the Pockels element). Depending on the magnitude of E, the polarization plane angle of the light from the polarizer 20 is changed by θ. The light that has passed through the electric field detection section 21 is applied to an analyzer 22 whose polarization plane has a predetermined relationship with the polarization plane of the polarizer 20, and the light that has passed through the analyzer 22 is sent to a light receiving section that outputs an electric signal according to the amount of light. Added. As shown in FIG. 5, when the degree of vacuum in the vacuum chamber or disconnector is good, the electric field E near the outside of the shield 9 is small, and as the degree of vacuum deteriorates, the electric field E increases. Therefore, the change angle θ of the polarization plane of light in the electric field detection unit 21 is small when the degree of vacuum is good;
When the degree of vacuum becomes poor, θ increases. Therefore, if the polarization plane of the analyzer 22 and the polarization plane of the polarizer 20 are at right angles, if the degree of vacuum becomes poor, the analyzer 22
The amount of light passing through increases, and the output A of the light receiving section 24 increases.
increases as shown by the solid line in FIG. Furthermore, when the polarization planes of the analyzer 22 and the polarizer 20 are parallel, if the degree of vacuum becomes poor, the amount of light passing through the analyzer 22 will decrease, and the output A of the light receiving section 24 will be as shown by the dotted line in FIG. becomes smaller. Therefore, deterioration in the degree of vacuum can be detected when the output of the light receiving section 24 suddenly increases or decreases.
第6図は本発明の第1の実施例を示し、25は
水平方向に設置された真空しや断器26の周囲を
モールドした固体絶縁部材で、固体絶縁部材25
のシールド9の外周下部に対応した部分に穴25
aを半径方向(上下方向)に設け、この穴25a
に電界検知部21として両側面が傾斜した屋根形
の電気光学効果素子(ポツケルス素子又はカー素
子)27を真空しや断器26側が先細側となるよ
うに支持させ、その下方には電気光学効果素子2
7に光を送る偏光子20、該素子27からの光を
受ける検光子22、偏光子20に光を送る光源2
3および検光子22からの光を受ける受光部24
を適宜設け、又受光部24には真空度良否判定部
28を電気的に接続する。この例では、光源23
からの光は偏光子20を介して素子27に加えら
れ、素子27では二つの傾斜面で光が反射するた
めその入力光と出力光は平行となり、出力光は検
光子22を介して受光部24に加えられる。従つ
て、真空しや断器26の真空度が劣化すると素子
27に対する印加電界が大きく変化するため受光
部24の出力が大きく変化し、この変化により真
空度良否判定部28は真空度劣化を検知して警報
や表示のための出力を出す。 FIG. 6 shows a first embodiment of the present invention, in which numeral 25 denotes a solid insulating member molded around a vacuum shield breaker 26 installed horizontally;
A hole 25 is formed in the part corresponding to the lower outer periphery of the shield 9.
a is provided in the radial direction (vertical direction), and this hole 25a
A roof-shaped electro-optic effect element (Pockels element or Kerr element) 27 with sloped sides is supported as the electric field detection part 21 so that the vacuum shield breaker 26 side is the tapered side, and below it is an electro-optic effect element. Element 2
a polarizer 20 that sends light to the element 7; an analyzer 22 that receives light from the element 27; a light source 2 that sends light to the polarizer 20;
3 and a light receiving section 24 that receives light from the analyzer 22.
are provided as appropriate, and a degree of vacuum quality determination section 28 is electrically connected to the light receiving section 24. In this example, the light source 23
The light is applied to the element 27 via the polarizer 20, and in the element 27, the light is reflected by two inclined surfaces, so the input light and output light become parallel, and the output light passes through the analyzer 22 to the light receiving section. Added to 24. Therefore, when the degree of vacuum of the vacuum chamber breaker 26 deteriorates, the electric field applied to the element 27 changes greatly, and the output of the light receiving section 24 changes greatly, and based on this change, the degree of vacuum quality judgment section 28 detects the deterioration of the degree of vacuum. and output for alarms and displays.
第7図は本発明の第2の実施例を示し、この例
では光源としてビーム拡りが小さく直線性の良い
レーザ29を用いており、光を効率良く用いるこ
とができるとともにレーザ29が既に直線偏光さ
れている場合には偏光子20を省略することがで
きる。 FIG. 7 shows a second embodiment of the present invention. In this example, a laser 29 with small beam spread and good linearity is used as a light source, and the light can be used efficiently and the laser 29 is already in a straight line. If the light is polarized, the polarizer 20 can be omitted.
第8図は本発明の第3の実施例を示し、この例
では電界検知部21を直方体の電気光学効果素子
30とその両側に密着した直角プリズム31,3
2とから形成しており、電界検知部21に対する
入力光と出力光が平行となるように直角プリズム
31,32により光を屈折させている。 FIG. 8 shows a third embodiment of the present invention, in which the electric field detection section 21 is formed by a rectangular parallelepiped electro-optic effect element 30 and right-angled prisms 31 and 3 closely attached to both sides thereof.
2, and the light is refracted by right angle prisms 31 and 32 so that the input light and output light to the electric field detection section 21 are parallel.
第9図は本発明の第4の実施例を示し、この例
では電界検知部21を直方体の電気光学効果素子
33とその真空しや断器26側に密着した誘電体
反射膜34とから形成しており、この誘電体反射
膜34により入力光を反射させるようにしたもの
である。 FIG. 9 shows a fourth embodiment of the present invention, in which the electric field detection section 21 is formed from a rectangular parallelepiped electro-optic effect element 33 and a dielectric reflective film 34 that is in close contact with the vacuum shield and the breaker 26 side. The dielectric reflective film 34 reflects input light.
第10図および11図は夫々本発明の第5およ
び第6の実施例を示し、これらの例では穴25a
内に設置された素子27,33の光入出力側に偏
光子20および検光子22を密着してこれらの間
の光伝送系における偏光面の歪を除去するととも
に、光源23と偏光子20の間および検光子22
と受光部24の間の光伝送を夫々光フアイバー3
5,36により行うことにより光損失を少くして
光源として光パワーは弱いが安価で信頼性が高い
発光ダイオードの使用を可能としている。尚、光
フアイバー35,36は光パワーの伝送のみに使
用されるのでマルチモードの光フアイバーで良
い。 FIGS. 10 and 11 show fifth and sixth embodiments of the invention, respectively, in which the holes 25a
A polarizer 20 and an analyzer 22 are placed in close contact with the light input and output sides of the elements 27 and 33 installed in the interior to eliminate distortion of the plane of polarization in the optical transmission system between them, and also to between and analyzer 22
The optical fiber 3 transmits light between the
5 and 36, it is possible to reduce optical loss and use a light emitting diode, which has low optical power but is inexpensive and highly reliable, as a light source. Note that since the optical fibers 35 and 36 are used only for transmitting optical power, they may be multi-mode optical fibers.
又、電気光学効果素子27,30,33として
は絶縁上からは固体絶縁部材25(比誘電率約
4)と比誘電率がほぼ等しい水晶(比誘電率4、
3)が良いが、感度の点からは電界集中効果によ
り等価的に感度が良くなる比誘電率の高いもの例
えばADP、KDP(比誘電率40〜50)が良い。た
だし、比誘電率が極端に高いものを用いると絶縁
破壊を生ずる。 In addition, the electro-optic effect elements 27, 30, and 33 are made of quartz crystal (relative permittivity: 4,
3) is better, but from the viewpoint of sensitivity, it is better to use a material with a high dielectric constant, such as ADP or KDP (relative dielectric constant 40 to 50), which equivalently improves sensitivity due to the electric field concentration effect. However, if a material with an extremely high dielectric constant is used, dielectric breakdown will occur.
上記の第1〜6の実施例では、真空しや断器2
6をモールドした固体絶縁部材25に穴25aを
設け、この穴25aに電界検知部21を設置した
ので電界検知部21の支持手段を特に設ける必要
がない。又、このように穴25aに電界検知部2
1の設置が可能となつたのは電界検知部21にお
いて光を入力方向側に反射させるようにしたため
で、又このように反射構造としたために素子2
7,30,33における光路長が長くなり、電界
による偏光面の変化角θが大きくなつて(変化角
θは電界Eと光路長Lに対応して変化する。)電
界検知の感度が良好となる。 In the first to sixth embodiments described above, the vacuum shield breaker 2
Since the hole 25a is provided in the solid insulating member 25 molded with 6 and the electric field detection section 21 is installed in the hole 25a, there is no need to provide any special support means for the electric field detection section 21. Moreover, the electric field detection part 2 is inserted into the hole 25a in this way.
1 was made possible because the electric field detection section 21 reflected the light toward the input direction, and because of this reflective structure, the installation of element 2 was made possible.
The optical path lengths at 7, 30, and 33 become longer, and the angle of change θ of the plane of polarization due to the electric field becomes larger (the angle of change θ changes in accordance with the electric field E and the optical path length L), and the sensitivity of electric field detection is improved. Become.
以上のように本発明に係る真空度監視装置は光
源と、光源からの光を直線偏光する偏光子と、偏
光子からの光の偏光面角度を印加電界の大きさに
応じて変化させる電界検知部と、偏光子の偏光面
と所定な関係にある偏光面を有するとともに電界
検知部からの光を受ける検光子とから成り、少く
ともその電界検知部は真空開閉器の真空度によつ
て電界が変化する位置で真空開閉器の周囲をモー
ルドした固体絶縁部材に真空開閉器外周位置で外
部側から設けた穴内に支持している。このため、
真空開閉器は真空度が劣化するとその外側の電界
が変化するので、電界検知部における光の偏光面
角度が変化し、検光子の通過光量が変化する。従
つてこの通過光量の変化から真空開閉器の開極時
および閉極時にかかわらず真空度の劣化を検知す
ることができ、真空度を常時監視することができ
る。又、真空度監視装置は上記のような構成であ
るので構成が簡単であり、光源、偏光子、検光子
および電界検知部はいずれも小形で安価なもので
あるため真空度監視装置も小形で安価なものとな
る。又、偏光子、検光子および電界検知部はいず
れも絶縁材であるのでこれらの部材を真空開閉器
の周囲に設けても絶縁上何ら支障はない。さら
に、少くとも電界検知部は真空開閉器の周囲をモ
ールドする固体絶縁部材の穴内に支持しているの
で特別な支持手段を要しないとともに真空開閉器
に近づくため電界検知感度が向上する。又、電界
検知部の真空開閉器側に光の反射面を設けたので
偏光子からの光は電界検知部内を往復してその光
路長が長くなり、電界検知感度が向上する。 As described above, the vacuum level monitoring device according to the present invention includes a light source, a polarizer that linearly polarizes the light from the light source, and an electric field sensor that changes the polarization plane angle of the light from the polarizer according to the magnitude of the applied electric field. and an analyzer which has a polarization plane in a predetermined relationship with the polarization plane of the polarizer and which receives light from the electric field detection section. The vacuum switch is supported in a hole formed from the outside at a position on the outer periphery of the vacuum switch in a solid insulating member molded around the vacuum switch at a position where the pressure changes. For this reason,
When the degree of vacuum in a vacuum switch deteriorates, the electric field outside the switch changes, so the polarization plane angle of light in the electric field detection section changes, and the amount of light passing through the analyzer changes. Therefore, deterioration in the degree of vacuum can be detected from changes in the amount of passing light regardless of whether the vacuum switch is opened or closed, and the degree of vacuum can be constantly monitored. In addition, the vacuum level monitoring device has the above-mentioned configuration, so the configuration is simple, and the light source, polarizer, analyzer, and electric field detection unit are all small and inexpensive, so the vacuum level monitoring device is also small. It will be cheap. Furthermore, since the polarizer, analyzer, and electric field detection section are all made of insulating materials, there is no problem in terms of insulation even if these members are provided around the vacuum switch. Furthermore, since at least the electric field detection section is supported within the hole of the solid insulating member molded around the vacuum switch, no special supporting means is required, and the electric field detection sensitivity is improved because it is close to the vacuum switch. Furthermore, since a light reflecting surface is provided on the vacuum switch side of the electric field detection section, the light from the polarizer travels back and forth within the electric field detection section, increasing the optical path length and improving electric field detection sensitivity.
第1図A,Bおよび第2図は夫々真空しや断器
の通電状態における縦断正面図、等価回路図およ
び真空度と各部の電圧、電界との関係図、第3図
A,Bは夫々真空しや断器のしや断状態における
縦断正面図および等価回路図、第4、5図は夫々
本発明に係る真空度監視装置の基本的構成図およ
び真空度と電界、受光部出力との関係図、第6〜
11図は夫々本発明の第1〜6の実施例に係る真
空度監視装置の構成図。
20……偏光子、21……電界検知部、22…
…検光子、23……光源、24……受光部、25
……固体絶縁部材、25a……穴、26……真空
しや断器、27,30,33……電気光学効果素
子、31,32……直角プリズム、34……誘電
体反射膜。
Figures 1A and B and Figure 2 are respectively a longitudinal sectional front view of the vacuum shield breaker in the energized state, an equivalent circuit diagram, and a diagram of the relationship between the degree of vacuum and the voltage and electric field of each part, and Figures 3A and B are respectively Figures 4 and 5 are a longitudinal sectional front view and an equivalent circuit diagram of the vacuum shield and breaker in the shielded state, respectively, and a basic configuration diagram of the vacuum degree monitoring device according to the present invention, and the relationship between the degree of vacuum, the electric field, and the output of the light receiving section. Relationship diagram, 6th ~
FIG. 11 is a configuration diagram of a vacuum degree monitoring device according to the first to sixth embodiments of the present invention. 20...Polarizer, 21...Electric field detection section, 22...
...Analyzer, 23...Light source, 24...Light receiving section, 25
. . . Solid insulating member, 25a . . . Hole, 26 . . . Vacuum shield breaker, 27, 30, 33 .
Claims (1)
開閉器において、光源と光源からの光を直線偏光
する偏光子と偏光子からの光の偏光面角度を印加
電界の大きさに応じて変化させる電界検知部と偏
光子の偏光面と所定な関係にある偏光面を有する
とともに電界検知部からの光を受ける検光子とを
備え、少くとも前記電界検知部は真空開閉器外周
において前記固体絶縁部材に外部側から設けた穴
内に支持し、かつ前記電界検知部はその真空開閉
器側に光の反射面を有するものとしたことを特徴
とする真空開閉器の真空度監視装置。1 In a vacuum switch whose periphery is molded with a solid insulating material, a light source, a polarizer that linearly polarizes the light from the light source, and an electric field detection unit that changes the polarization plane angle of the light from the polarizer according to the magnitude of the applied electric field. and an analyzer that has a polarization plane in a predetermined relationship with the polarization plane of the polarizer and receives light from the electric field detection section, and at least the electric field detection section is connected to the solid insulating member on the outer periphery of the vacuum switch. 1. A degree of vacuum monitoring device for a vacuum switch, characterized in that the electric field detection section has a light reflecting surface on the side of the vacuum switch.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5278881A JPS57168434A (en) | 1981-04-08 | 1981-04-08 | Vacuum degree monitoring device for vacuum switch |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5278881A JPS57168434A (en) | 1981-04-08 | 1981-04-08 | Vacuum degree monitoring device for vacuum switch |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57168434A JPS57168434A (en) | 1982-10-16 |
| JPH0121573B2 true JPH0121573B2 (en) | 1989-04-21 |
Family
ID=12924569
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5278881A Granted JPS57168434A (en) | 1981-04-08 | 1981-04-08 | Vacuum degree monitoring device for vacuum switch |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57168434A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE19540399B4 (en) * | 1995-10-30 | 2004-09-16 | Daimlerchrysler Ag | Center console for a motor vehicle |
| CN102607768A (en) * | 2012-04-01 | 2012-07-25 | 常熟市虞华真空设备科技有限公司 | Calibration device used for experiment |
-
1981
- 1981-04-08 JP JP5278881A patent/JPS57168434A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57168434A (en) | 1982-10-16 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US4999571A (en) | Current and/or voltage detector for a distribution system | |
| KR0173672B1 (en) | Fiber optic device for measuring current strength | |
| US6016053A (en) | Gas-insulated switchgear with voltage transformer and optical measuring element | |
| JPH0121573B2 (en) | ||
| JPH1114669A (en) | Electrooptical sensor having solid voltage divider | |
| JPS648413B2 (en) | ||
| JP3489701B2 (en) | Electric signal measuring device | |
| JPS644205Y2 (en) | ||
| JPS644202Y2 (en) | ||
| JPS644201Y2 (en) | ||
| JPS6022288B2 (en) | Vacuum level monitoring device for vacuum electrical equipment | |
| JPH08211107A (en) | Optical voltage measuring device for gas-insulated electrical equipment | |
| JPH0562569A (en) | Vacuum degree monitoring device for vacuum switchgear | |
| US11486906B2 (en) | Voltage measuring device and gas-insulated switching apparatus | |
| JPS6148856B2 (en) | ||
| JPS6322505Y2 (en) | ||
| JPS644203Y2 (en) | ||
| JPS644204Y2 (en) | ||
| JPS6310773B2 (en) | ||
| KR860001475B1 (en) | Vacuum degree monitoring device of vacuum electric equipment | |
| JPS6324422Y2 (en) | ||
| JP2969035B2 (en) | Optical PT | |
| US3551679A (en) | Low drive power wideband optical modulator | |
| JP2921367B2 (en) | Optical voltmeter | |
| JP2595162Y2 (en) | Optical surge voltage sensor |