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JPH0515988B2 - - Google Patents
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JPH0515988B2 - - Google Patents

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Publication number
JPH0515988B2
JPH0515988B2 JP57226268A JP22626882A JPH0515988B2 JP H0515988 B2 JPH0515988 B2 JP H0515988B2 JP 57226268 A JP57226268 A JP 57226268A JP 22626882 A JP22626882 A JP 22626882A JP H0515988 B2 JPH0515988 B2 JP H0515988B2
Authority
JP
Japan
Prior art keywords
electric field
light
electro
section
detection section
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 - Lifetime
Application number
JP57226268A
Other languages
Japanese (ja)
Other versions
JPS59116555A (en
Inventor
Kazuyuki Nagatsuma
Hiroyoshi Matsumura
Yasuo Suganuma
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.)
Hitachi Cable Ltd
Hitachi Ltd
Original Assignee
Hitachi Cable Ltd
Hitachi 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 Hitachi Cable Ltd, Hitachi Ltd filed Critical Hitachi Cable Ltd
Priority to JP57226268A priority Critical patent/JPS59116555A/en
Publication of JPS59116555A publication Critical patent/JPS59116555A/en
Publication of JPH0515988B2 publication Critical patent/JPH0515988B2/ja
Granted legal-status Critical Current

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  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
  • Measurement Of Current Or Voltage (AREA)

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は電気光学効果を利用した電界測定装置
に係り、特に直流電界を測定する光方式電界測定
装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an electric field measuring device that utilizes an electro-optical effect, and particularly to an optical electric field measuring device that measures a direct current electric field.

〔従来技術〕[Prior art]

従来の、電気光学効果を有する媒質(以下、電
気光学結晶と記す)を利用した電圧測定装置、電
界測定装置の測定対象は、ほとんどの場合交流電
圧、交流電界に限られている。その理由は、直流
電界中に電気光学結晶を静置すると、一般的に、
その静電容量、直流抵抗が大きいため時間ととも
に測定値が変化し、さらに結晶表面に電荷集中が
起り、いわゆる表面層が形成されて、測定不能と
なるからである。
Conventional voltage measuring devices and electric field measuring devices that utilize a medium having an electro-optic effect (hereinafter referred to as an electro-optic crystal) are mostly limited to alternating current voltages and alternating electric fields. The reason is that when an electro-optic crystal is placed in a DC electric field, generally
This is because the measured value changes over time due to its large capacitance and DC resistance, and charge concentration occurs on the crystal surface, forming a so-called surface layer, making measurement impossible.

上記従来の、電気光学結晶を利用した電界測定
装置(以下、光方式電界強度測定器と記す)で
は、交流電界中に電気光学結晶を静置し、電界の
変化に従つてその結晶中に誘起される複屈折変化
を、偏光子、検光子等を用いて光強度信号(但し
交流信号である)として検出し電界の変化を測定
している。その詳細は、例えば、「公開特許公報
特開昭56−100364号、「電子通信学会技術研究報
告、Vol.80、No.6(1980)、第19頁〜第24頁、
OQE80−4、光応用電界センサ」等に記載され
ている。
In the above-mentioned conventional electric field measuring device using an electro-optic crystal (hereinafter referred to as an optical field strength measuring device), the electro-optic crystal is placed in an alternating current electric field, and the electro-optic crystal is placed in an alternating current electric field. The change in birefringence caused by this is detected as a light intensity signal (alternating current signal) using a polarizer, analyzer, etc., and the change in the electric field is measured. For details, see, for example, "Public Patent Publication No. 56-100364, IEICE Technical Research Report, Vol. 80, No. 6 (1980), pp. 19 to 24.
OQE80-4, Optical Applied Electric Field Sensor, etc.

本発明者らは、先に、電気光学効果を利用した
電界測定装置の測定対象を直流電界へも拡張する
方法として、1 電気光学結晶自体を回転する方
法、2 光導電効果を利用して充電電荷を断続的
に中和する方法を考案し、それぞれ出願した。し
かしながら、上記2方法においても、それぞれ、
1 電気光学結晶が回転しても光透過量が変化し
ないように、結晶加工および回転機構を精密化す
る、2 光導電体の有効的な抵抗値が、光の非照
射時に、十分大きいよう高品質化するなどの実用
上の問題点が存在し、改善策が望まれている。
The present inventors previously proposed two methods for extending the measurement target of an electric field measurement device using the electro-optic effect to include DC electric fields: 1. A method of rotating the electro-optic crystal itself; 2. Charging using the photoconductive effect They devised a method to neutralize the electric charge intermittently and filed applications for each method. However, in the above two methods, respectively,
1. The crystal processing and rotation mechanism are refined so that the amount of light transmitted does not change even when the electro-optic crystal is rotated. 2. The effective resistance value of the photoconductor is made high enough to be large enough when not irradiated with light. There are practical problems such as quality issues, and improvement measures are desired.

〔発明の目的〕[Purpose of the invention]

本発明は、従来の光方式電界強度測定器におけ
る上記難点を解消し、直流電界の強さの測定を可
能ならしめる新らたな光方式直流電界測定装置の
提供を目的とするものである。
SUMMARY OF THE INVENTION An object of the present invention is to provide a new optical DC electric field measuring device that overcomes the above-mentioned difficulties in conventional optical electric field strength measuring devices and makes it possible to measure the strength of a DC electric field.

〔発明の概要〕[Summary of the invention]

上記目的を達成するため、本発明の光方式直流
電界測定装置は、光源部、該光源部からの光の強
度を電界強度の対応して変化せしめる電界検出
部、該検出部からの光の強度を計測する計測部、
ならびに該光源部と該検出部および該計測部を光
学的に結合する伝送路を有し、該検出部が、電気
光学結晶と回転スイツチの両者を具備している。
In order to achieve the above object, the optical DC electric field measurement device of the present invention includes a light source section, an electric field detection section that changes the intensity of light from the light source section in accordance with the electric field intensity, and an electric field detection section that changes the intensity of light from the detection section. a measurement unit that measures
It also has a transmission path that optically couples the light source section, the detection section, and the measurement section, and the detection section includes both an electro-optic crystal and a rotary switch.

回転スイツチは、前記電気光学結晶の表面にお
ける前記電荷集中による充電電荷を断続的に中和
するためのものである。この回転スイツチとして
は、電動モータなどの外部電源を要する電気的ス
イツチよりも、電気をみださない気流体を利用し
た回転スイツチが望ましい。また、この気流体と
して温度制御された気流体を使用すると、電気光
学結晶を温度制御することができ有用である。
The rotary switch is for intermittently neutralizing the charge caused by the charge concentration on the surface of the electro-optic crystal. As this rotary switch, a rotary switch that uses air and fluid, which does not emit electricity, is preferable to an electric switch that requires an external power source such as an electric motor. Furthermore, it is useful to use a temperature-controlled gas fluid as the gas fluid because the temperature of the electro-optic crystal can be controlled.

本光方式直流電界測定装置の電界検出部におい
て、電気光学結晶の2表面は電極付されており、
測定時、印加直流電界に対し垂直に配置される。
回転体スイツチは電気光学結晶の近傍に設置さ
れ、両者は、導電体により接続される。回転体ス
イツチが投入時、電界に対し垂直な2表面間は短
絡され、2表面の電荷は中和される。一方、開放
時は、電気光学結晶に電界が印加され、電気光学
効果が誘起されて、測定状態となる。
In the electric field detection section of this optical DC electric field measurement device, two surfaces of the electro-optic crystal are provided with electrodes.
During measurement, it is placed perpendicular to the applied DC electric field.
The rotary switch is installed near the electro-optic crystal, and both are connected by a conductor. When the rotary switch is turned on, the two surfaces perpendicular to the electric field are short-circuited, and the charges on the two surfaces are neutralized. On the other hand, when it is open, an electric field is applied to the electro-optic crystal, an electro-optic effect is induced, and a measurement state is established.

この投入状態と開放状態の時間(開放時間、投
入時間)は、回転体スイツチの形状および回転速
度により制御される。
The time between the closing state and the opening state (opening time, closing time) is controlled by the shape and rotation speed of the rotary switch.

投入状態の上限は特に限定されないが、投入時
は電気光学効果による出力は消失するので、測定
の便宜を考えて定めることになる。また投入時間
をあまり短かくすると充電電荷を十分に放電でき
なくなり支障を生じるので、その下限が存在する
ことになるが、これは簡単な実験により支障のな
い投入時間を確認すればよい。また開放時間の上
限は、前記充電電荷により電界強度の測定が不可
能になる時間であり、必要に応じて簡単な実験に
より定めることができる。開放時間の下限は特に
存在しないが、あまり短かくすると電界強度の測
定に支障を来すことになるので、支障を生じない
範囲の開放時間とする。
The upper limit of the closed state is not particularly limited, but since the output due to the electro-optic effect disappears when the capacitor is closed, it is determined in consideration of the convenience of measurement. Furthermore, if the charging time is too short, the charged charge cannot be sufficiently discharged, causing a problem, so a lower limit exists, but this can be determined by a simple experiment to confirm the charging time without causing any problems. Further, the upper limit of the open time is the time during which it becomes impossible to measure the electric field intensity due to the charged charges, and can be determined by a simple experiment if necessary. There is no particular lower limit for the open time, but if it is too short, it will cause trouble in measuring the electric field strength, so the open time is set within a range that does not cause any trouble.

前記光伝送路には、周知のように光フアイバを
用いるのが好都合である。
As is well known, it is convenient to use an optical fiber as the optical transmission line.

前記光源部は、通常、発光ダイオードおよびそ
の励起電源などより成る。
The light source section usually includes a light emitting diode and an excitation power source for the light emitting diode.

前記電界検出部は、通常、光源部側の光フアイ
バと計測部側の光フアイバの間に、レンズ、偏光
子、電気光学結晶、検光子、レンズの順に、およ
び前述のごとく、電気光学結晶と並列に回転スイ
ツチが、配置されている。また、上記電気光学結
晶と検光子の間には、必要に応じてλ/4板を入
れる。検光子には、通常の検光子の他に、例えば
ウオラストンプリズムのような偏光プリズムを用
いてもよい。出射光側のレンズは、通常の検光子
の場合は1個、偏光プリズムの場合は2つの直線
偏光に分離するので2個とする。前記検出部から
出射された光は光フアイバで計測部の受光器に導
かれ、出力電気信号となる。この出力電気信号を
そのまま測定してもよいし、また光源部と電気光
学結晶との間で分岐された光(電気光学結晶を通
らない光)と検出部からの光とをそれぞれ受光器
で電気信号に変換し、両電気信号を演算装置に入
れ、電界強度を算出してもよい。また、偏光プリ
ズムを検光子として用いた場合には、出射光が2
偏光光線に分離するので、双方をそれぞれ受光器
で電気信号に変換し、両電気信号を演算装置に入
れて電界強度を算出する。なお、上記入射光側と
出射光側のレンズは省略することも可能である。
The electric field detection section usually includes a lens, a polarizer, an electro-optic crystal, an analyzer, and a lens, in this order, between the optical fiber on the light source side and the optical fiber on the measuring section side, and as described above, the electro-optic crystal and the optical fiber. Rotary switches are arranged in parallel. Further, a λ/4 plate is inserted between the electro-optic crystal and the analyzer, if necessary. In addition to a normal analyzer, a polarizing prism such as a Wollaston prism may be used as the analyzer. The number of lenses on the output light side is one in the case of a normal analyzer, and two in the case of a polarizing prism because the light is separated into two linearly polarized lights. The light emitted from the detection section is guided to the light receiver of the measurement section through an optical fiber, and becomes an output electrical signal. This output electrical signal may be measured as is, or the light branched between the light source section and the electro-optic crystal (light that does not pass through the electro-optic crystal) and the light from the detection section may be measured using an optical receiver. The electric field strength may be calculated by converting it into a signal and inputting both electric signals to a calculation device. Furthermore, when a polarizing prism is used as an analyzer, the output light is
Since it is separated into polarized light beams, both are converted into electrical signals by a photoreceiver, and both electrical signals are input into a calculation device to calculate the electric field strength. Note that the lenses on the incident light side and the exit light side may be omitted.

いずれにしても、本発明の光方式直流電界測定
装置は、電界検出部において、電気光学結晶の電
界印加方法と垂直な2面間に、気体流などによつ
て開閉(開放、投入)される回転スイツチが並列
に挿入されることが重要な点であり、他の構成に
ついては従来技術を踏襲して差支えない。
In any case, in the optical DC electric field measurement device of the present invention, in the electric field detection section, the electro-optic crystal is opened and closed (opened and closed) between two planes perpendicular to the electric field application method using a gas flow or the like. It is important that the rotary switches are inserted in parallel, and other configurations may follow the conventional technology.

〔発明の実施例〕[Embodiments of the invention]

以下、実施例により本発明をさらに詳細に説明
する。
Hereinafter, the present invention will be explained in more detail with reference to Examples.

第1図は、本実施例における光方式電界強度測
定器の構成図でああ。光源部1、電界検出部2、
計測部3、およびそれらを結合する光伝送路4−
1,4−2,4−3より構成されている。光源部
1は、0.83μmの波長の光を出射する発光ダイオ
ード1−1、およびその励起電源1−2、電界検
出部2は、ロツドレンズ2−1,2−2,23、
偏光子5、ウオラストンプリズム6、電気光学結
晶7、回転スイツチ8、導体9−1,9−2、気
体流導入パイプ10、気体流流出口11などより
成り立つている。測定部3はPINフオトダイオー
ド3−1,3−2および電気的な演算表示回路3
0よりなり、光伝送路4−1,4−2,4−3に
は、コア径500μmの、石英コア、プラスチツク
クラツドの光フアイバを使用している。
FIG. 1 is a configuration diagram of the optical field strength measuring device in this embodiment. light source section 1, electric field detection section 2,
Measurement unit 3 and optical transmission line 4- that connects them
It is composed of 1, 4-2, and 4-3. The light source section 1 includes a light emitting diode 1-1 that emits light with a wavelength of 0.83 μm and its excitation power source 1-2, and the electric field detection section 2 includes rod lenses 2-1, 2-2, 23,
It consists of a polarizer 5, a Wollaston prism 6, an electro-optic crystal 7, a rotary switch 8, conductors 9-1, 9-2, a gas flow introduction pipe 10, a gas flow outlet 11, and the like. The measuring section 3 includes PIN photodiodes 3-1, 3-2 and an electrical calculation display circuit 3.
For the optical transmission lines 4-1, 4-2, and 4-3, optical fibers with a core diameter of 500 μm, a quartz core, and a plastic cladding are used.

第2図は、第1図の電界検出部における回転ス
イツチ8、電気光学結晶7の構成関係、および回
転スイツチ8と導体9−1,9−2の構成関係を
示す説明図である。
FIG. 2 is an explanatory diagram showing the structural relationship between the rotary switch 8 and the electro-optic crystal 7 in the electric field detection section of FIG. 1, and the structural relationship between the rotary switch 8 and the conductors 9-1 and 9-2.

電源部1において、励起電源1−2により励起
された発光ダイオード1−1の光は光フアイバ4
−1により、電界検出部2に導びかれる。電界検
出部2において、偏光子5の光の振動方向(直線
偏光の向き)とウオラストンプリズム6の主軸の
なす角度は45度に設定されている。光フアイバケ
ーブル4−1より導びかれた光線はロツドレンズ
2−1、偏光子5で直線偏光の平行光線となり、
電気光学結晶7に入射する。電気光学結晶7では
電界Eの強度に応じて、その複屈析楕円体の楕円
率が変化するため、電気光学結晶7からは楕円偏
光の平行光線として出射される。その出射光はウ
オラストンプリズム6に導びかれ、2つの直角成
分の直線偏光となり、ロツドレンズ2−2,2−
3、光フアイバケーブル4−2,4−3を経て、
PINフオトダイオード3−1,3−2に導びか
れ、電気信号P1,P2に位変換される。電気的な
演算表示回路30では、 S=P1−P2/P1+P2 なる演算を行い、外部電界強度に応じた、電圧値
を表示する。
In the power supply unit 1, the light from the light emitting diode 1-1 excited by the excitation power supply 1-2 is transmitted through the optical fiber 4.
-1, it is guided to the electric field detection section 2. In the electric field detection unit 2, the angle between the vibration direction of the light of the polarizer 5 (direction of linearly polarized light) and the principal axis of the Wollaston prism 6 is set to 45 degrees. The light beam guided from the optical fiber cable 4-1 becomes a linearly polarized parallel light beam by the rod lens 2-1 and the polarizer 5.
The light is incident on the electro-optic crystal 7. In the electro-optic crystal 7, the ellipticity of the birefringence ellipsoid changes depending on the intensity of the electric field E, so that light is emitted from the electro-optic crystal 7 as parallel elliptically polarized light. The emitted light is guided to the Wollaston prism 6, where it becomes linearly polarized light with two orthogonal components, and rod lenses 2-2, 2-
3. Via optical fiber cables 4-2 and 4-3,
The signals are led to PIN photodiodes 3-1 and 3-2 and converted into electric signals P1 and P2 . The electrical calculation display circuit 30 performs the calculation S=P 1 -P 2 /P 1 +P 2 and displays a voltage value according to the external electric field strength.

電界検出部において、電気光学結晶7の電界E
に垂直な2面上には電極7−1,7−2が、真空
蒸着により付けられている。電気光学結晶7と、
回転スイツチ8とは導体9−1,9−2で接続さ
れており、回転スイツチ8は回転保持具12によ
り保持されている。導体9−1,9−2の間の電
位差は、回転スイツチ8に設けられた短絡電極1
3により、回転スイツチ8の回転に伴つて測定電
界に応じた有限値と零との間を断続する。
In the electric field detection section, the electric field E of the electro-optic crystal 7
Electrodes 7-1 and 7-2 are attached on two surfaces perpendicular to , by vacuum evaporation. electro-optic crystal 7,
It is connected to the rotary switch 8 through conductors 9-1 and 9-2, and the rotary switch 8 is held by a rotary holder 12. The potential difference between the conductors 9-1 and 9-2 is determined by the short-circuit electrode 1 provided on the rotary switch 8.
3, as the rotary switch 8 rotates, the electric field is switched between a finite value corresponding to the measured electric field and zero.

回転用気体流としては温度制御したN2ガス流
を用いた。
A temperature-controlled N 2 gas flow was used as the rotational gas flow.

本実施例では、回転スイツチの開閉周期は、ス
イツチ投入時(閉);約100ms、開放時(開);
約200msとした。
In this embodiment, the opening/closing cycle of the rotary switch is approximately 100 ms when the switch is turned on (closed), and approximately 100 ms when it is opened (opened);
It was set to about 200ms.

回転スイツチが開放時のみ、電界強度測定が可
能で、投入時には、電界強度測定は休止状態とな
る。なお第2図aのは光の進行方向を、bの
は回転スイツチの回転方向を示す。
Electric field strength measurement is possible only when the rotary switch is open, and when the rotary switch is turned on, field strength measurement is in a paused state. Note that FIG. 2a shows the traveling direction of the light, and FIG. 2b shows the rotating direction of the rotary switch.

電気光学結晶7としては、Bi12SiO20単結晶を
使用した。結晶は(110)、(110)、(001)面を
有しており、外形は5×5×5mmである。電界は
(110)方向に印加し、光は(110)方向に伝搬
させた。
As the electro-optic crystal 7, a Bi 12 SiO 20 single crystal was used. The crystal has (110), (110), and (001) planes, and the external size is 5 x 5 x 5 mm. An electric field was applied in the (110) direction, and light was propagated in the (110) direction.

第3図に、実際の電界強度測定結果を示す。第
3図は、直流電界強度と演算表示回路電気出力が
良好な直線関係を有することを示しており、本発
明により、直流電界の測定が可能であることが明
らかである。
FIG. 3 shows actual electric field strength measurement results. FIG. 3 shows that there is a good linear relationship between the DC electric field strength and the electrical output of the arithmetic display circuit, and it is clear that the present invention makes it possible to measure the DC electric field.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、従来不可能であつた直流電界
の測定が可能となる効果がある。
According to the present invention, there is an effect that it becomes possible to measure a direct current electric field, which was previously impossible.

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

第1図は本発明の一実施例における光方式直流
電界測定装置の構成全体を示す説明図、第2図a
は回転スイツチと電気光学結晶の構成関係を示す
説明図、第2図bは回転スイツチと導体の構成関
係を示す説明図、第3図は本発明の一実施例にお
ける光方式直流電界測定装置による直流電界強度
の測定結果を示すグラフである。 1……光源部、1−1……発光ダイオード、1
−2……電源、2……電界検出部、2−1,2−
2,2−3,……ロツドレンズ、3……計測部、
3−1,3−2……PINフオトダイオード、4−
1,4−2,4−3……光フアイバ伝送路、5…
…偏光子、6……ウオラストンプリズム、7……
電気光学結晶、8……回転スイツチ、9−1,9
−2……導体、10……気体流導入パイプ、11
……気体流流出口、12……回転スイツチ保持
具、13……短絡電極、30……演算表示回路。
Fig. 1 is an explanatory diagram showing the entire configuration of an optical DC electric field measuring device according to an embodiment of the present invention, Fig. 2a
is an explanatory diagram showing the structural relationship between the rotary switch and the electro-optic crystal, FIG. 2b is an explanatory diagram showing the structural relationship between the rotary switch and the conductor, and FIG. It is a graph showing measurement results of DC electric field strength. 1... Light source section, 1-1... Light emitting diode, 1
-2... Power supply, 2... Electric field detection section, 2-1, 2-
2, 2-3, ... Rod lens, 3 ... Measuring section,
3-1, 3-2...PIN photodiode, 4-
1, 4-2, 4-3...optical fiber transmission line, 5...
...Polarizer, 6...Wollaston prism, 7...
Electro-optic crystal, 8...Rotary switch, 9-1, 9
-2...Conductor, 10...Gas flow introduction pipe, 11
... Gas flow outlet, 12 ... Rotary switch holder, 13 ... Short circuit electrode, 30 ... Arithmetic display circuit.

Claims (1)

【特許請求の範囲】 1 光源部、該光源部からの光の強度を電界強度
に対応して変化せしめる電界検出部、該電界検出
部からの光の強度を計測する計測部、ならびに該
光源部と該検出部および該計測部を光学的に結合
する光伝送路を有し、該検出部が、電気光学効果
を有する媒質と、該媒質表面近傍の充電電荷の少
なくとも一部を放電するための気体流により回転
する回転体を用いた回転スイツチとを具備してい
ることを特徴とする光方式直流電界測定装置。 2 特許請求の範囲第1項記載の光方式直流電界
測定装置において、上記気体流を温度制御する手
段を有することを特徴とする光方式直流電界測定
装置。
[Scope of Claims] 1. A light source section, an electric field detection section that changes the intensity of light from the light source section in accordance with electric field intensity, a measurement section that measures the intensity of light from the electric field detection section, and the light source section. and an optical transmission path that optically couples the detection section and the measurement section, and the detection section includes a medium having an electro-optic effect and a medium for discharging at least a portion of the charge near the surface of the medium. 1. An optical direct current electric field measuring device characterized by comprising a rotary switch using a rotating body rotated by a gas flow. 2. An optical direct current electric field measuring device according to claim 1, further comprising means for controlling the temperature of the gas flow.
JP57226268A 1982-12-24 1982-12-24 Optical type dc electric field measuring apparatus Granted JPS59116555A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57226268A JPS59116555A (en) 1982-12-24 1982-12-24 Optical type dc electric field measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57226268A JPS59116555A (en) 1982-12-24 1982-12-24 Optical type dc electric field measuring apparatus

Publications (2)

Publication Number Publication Date
JPS59116555A JPS59116555A (en) 1984-07-05
JPH0515988B2 true JPH0515988B2 (en) 1993-03-03

Family

ID=16842536

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57226268A Granted JPS59116555A (en) 1982-12-24 1982-12-24 Optical type dc electric field measuring apparatus

Country Status (1)

Country Link
JP (1) JPS59116555A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2986503B2 (en) * 1990-03-09 1999-12-06 株式会社日立製作所 Optical DC voltage transformer

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58174857A (en) * 1982-04-08 1983-10-13 Yokogawa Hokushin Electric Corp Dc photo/voltmeter

Also Published As

Publication number Publication date
JPS59116555A (en) 1984-07-05

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