JPH0835998A - Measuring instrument probe and voltage measuring method - Google Patents
Measuring instrument probe and voltage measuring methodInfo
- Publication number
- JPH0835998A JPH0835998A JP17065894A JP17065894A JPH0835998A JP H0835998 A JPH0835998 A JP H0835998A JP 17065894 A JP17065894 A JP 17065894A JP 17065894 A JP17065894 A JP 17065894A JP H0835998 A JPH0835998 A JP H0835998A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- optical modulator
- measuring instrument
- light
- voltage
- 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.)
- Pending
Links
Landscapes
- Measurement Of Current Or Voltage (AREA)
- Measuring Leads Or Probes (AREA)
Abstract
(57)【要約】
【目的】 改善された計測方法を可能とし,高周波はも
とより3相交流等の低周波多相信号に対しても十分な信
頼性を有する測定を可能ならしめる計測器用プローブと
電圧計測方法とを提供すること。
【構成】 計測器用プローブは,光変調器5と,導体
3,4と,入力光ファイバ12と,出力光ファイバ15
と光検出器16とを備えている。光変調器5は,二つの
電極間に印加される電圧に依存して前記電極の近傍を通
った光の強度を変化させる。また,導体3,4は,前記
電極に一端が接続され他端に検出端子1,2を備えてい
る。入力光ファイバ12は光源からの光を光変調器5に
伝搬する。出力光ファイバ15は前記光変調器からの光
出力を伝搬する。光検出器16は,出力光ファイバ15
に接続され電気出力を非対称計測器であるオシロスコー
プ19に接続するための同軸コネクタ17を持つ。この
計測器用プローブは,検出端子1,2を被測定点である
電気回路内の任意の2点に接触または保持する機能を有
する。
(57) [Abstract] [Purpose] A probe for a measuring instrument that enables an improved measurement method and that enables measurement with sufficient reliability not only for high frequencies but also for low-frequency polyphase signals such as three-phase AC. To provide a voltage measuring method. [Structure] The measuring instrument probe includes an optical modulator 5, conductors 3 and 4, an input optical fiber 12, and an output optical fiber 15.
And a photodetector 16. The light modulator 5 changes the intensity of light passing near the electrodes depending on the voltage applied between the two electrodes. The conductors 3 and 4 have one end connected to the electrode and the other end provided with detection terminals 1 and 2. The input optical fiber 12 propagates the light from the light source to the optical modulator 5. The output optical fiber 15 propagates the optical output from the optical modulator. The photodetector 16 has an output optical fiber 15
And a coaxial connector 17 for connecting an electric output to an oscilloscope 19 which is an asymmetric measuring instrument. This measuring instrument probe has a function of contacting or holding the detection terminals 1 and 2 at any two points in the electric circuit which are the points to be measured.
Description
【0001】[0001]
【産業上の利用分野】本発明は,電気回路内等における
電圧を計測するためのプローブと計測方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a probe and a measuring method for measuring a voltage in an electric circuit or the like.
【0002】[0002]
【従来の技術】従来,電気回路内部等における電圧波形
計測には,計測対象間にオシロスコープの測定用プロー
ブが用いられてきた。このプローブによって検出端の信
号を直接オシロスコープに導いて電圧波形を計測するも
ので,広く利用されている。2. Description of the Related Art Conventionally, an oscilloscope measuring probe has been used between measurement targets for measuring voltage waveforms inside an electric circuit or the like. This probe directly guides the signal at the detection end to an oscilloscope and measures the voltage waveform. It is widely used.
【0003】[0003]
【発明が解決しようとする課題】オシロスコープ等,従
来の電気式プローブから同軸ケーブルによって接続され
被測定点を計測器のアースと信号ラインに区別して測定
する非対称計測器では,計測器とグランドレベルが異な
る電気回路や,グランドされていない2点間の電圧波形
等を観測するとき,アースの影響や信号のまわりこみ,
さらにはプローブの容量等が影響し,正確な計測が困難
であるばかりでなく,不要な情報が計測されることがあ
り,測定対象が高周波の場合とくにこうした問題が解決
されないままになっていた。In an asymmetrical measuring instrument such as an oscilloscope which is connected by a coaxial cable from a conventional electric probe and which measures the point under measurement by distinguishing it between the measuring instrument ground and the signal line, the measuring instrument and the ground level are different from each other. When observing different electrical circuits or voltage waveforms between two points that are not grounded, the effects of grounding, signal sneaking,
Furthermore, due to the capacitance of the probe and other factors, accurate measurement is difficult, and unnecessary information may be measured. This problem remains unsolved especially when the measurement target is high frequency.
【0004】本発明の技術的課題は,かかる切望されて
いた課題を解決し,改善された計測方法を可能とし,高
周波はもとより3相交流等の低周波多相信号に対しても
十分な信頼性を有する測定を可能ならしめる計測器用プ
ローブと電圧計測方法とを提供することにある。The technical problem of the present invention is to solve such a long-awaited problem, to enable an improved measuring method, and to have a sufficient reliability not only for high frequencies but also for low frequency polyphase signals such as three-phase alternating current. An object of the present invention is to provide a measuring instrument probe and a voltage measuring method that enable accurate measurement.
【0005】[0005]
【課題を解決するための手段】前記課題を解決するため
の手段として,本発明では,被測定電圧を光変調器の電
極に印加し,前記電極の近傍を通り,前記被測定電圧に
依存して変化した光の強度を電気信号に変換した上で,
非対称計測器を用いて計測することを特徴とする電圧計
測方法である。As means for solving the above problems, in the present invention, a voltage to be measured is applied to an electrode of an optical modulator, passes through the vicinity of the electrode, and is dependent on the voltage to be measured. After converting the intensity of the changed light into an electric signal,
It is a voltage measuring method characterized by measuring using an asymmetrical measuring device.
【0006】また本発明の計測器用プローブは,二つの
電極間に印加される電圧に依存して前記電極の近傍を通
った光の強度を変化させる光変調器と,前記電極に一端
が接続され他端に検出端子を備えた導体と,光源からの
光を前記光変調器に伝搬する光入力部と,前記光変調器
からの光出力を伝搬する光出力部と,前記光出力部に接
続され電気出力を非対称計測器に接続するための同軸コ
ネクタを持つ光検出器とを備え,前記検出端子を被測定
点である電気回路内の任意の2点に接触または保持する
機能を有することを特徴としている。The measuring instrument probe of the present invention has an optical modulator for changing the intensity of light passing through the vicinity of the electrode depending on the voltage applied between the two electrodes, and one end of which is connected to the electrode. Connected to a conductor having a detection terminal at the other end, an optical input section for propagating light from a light source to the optical modulator, an optical output section for propagating an optical output from the optical modulator, and the optical output section A photodetector having a coaxial connector for connecting the electrical output to an asymmetrical measuring instrument, and having a function of contacting or holding the detection terminal at any two points in the electrical circuit which is the measured point. It has a feature.
【0007】また,本発明の計測器用プローブは,一つ
の端面から入射し,電圧を印加した二つの電極の近傍を
通り,他の端面で反射した後,さきに入射した前記端面
から出射する光の強度が,前記印加電圧に依存して変化
する光変調器と,前記電極に一端が接続され他端に検出
端子を備えた導体と,非対称計測器に接続するための同
軸コネクタを持つ光検出器及び前記光の光源を夫々付設
した光方向性分離器と,前記光方向性分離器及び前記光
変調器間を接続する入力及び出力伝達機能をもつ光伝搬
部とを備え,前記検出端子を被測定点である電気回路内
の任意の2点に接触または保持する機能を有することを
特徴としている。Further, the probe for a measuring instrument according to the present invention is a light which is incident from one end face, passes through the vicinity of two electrodes to which a voltage is applied, is reflected by the other end face, and is then emitted from the end face which is incident upon. Optical modulator having an optical modulator whose intensity changes depending on the applied voltage, a conductor having one end connected to the electrode and a detection terminal at the other end, and a coaxial connector for connecting to the asymmetric measuring instrument. Device and an optical directional separator each provided with a light source for the light, and an optical propagation section having an input and output transmission function for connecting the optical directional separator and the optical modulator, and the detection terminal It is characterized by having a function of contacting or holding two arbitrary points in the electric circuit, which is a measured point.
【0008】また,本発明の計測器用プローブにおい
て,前記光変調器は,非金属材料からなる容器に収容さ
れていることを特徴としている。The measuring instrument probe of the present invention is characterized in that the optical modulator is housed in a container made of a non-metallic material.
【0009】さらに,本発明の計測器用プローブにおい
て,前記光変調器はマッハツェンダ光干渉型光変調器で
あることを特徴としている。Further, in the measuring instrument probe of the present invention, the optical modulator is a Mach-Zehnder interferometric optical modulator.
【0010】[0010]
【作用】本発明による計測方法は,電圧が印加された二
つの電極の近傍を通った光を,電圧に依存して,受ける
作用を光の強度変化として検出し,これを電気信号に変
換して計測処理するものである。被測定点は計測器と電
気的に完全に分離されるので,前述のようなアースや電
気的なまわりこみの影響はすべて回避される。According to the measuring method of the present invention, the light passing through the vicinity of the two electrodes to which a voltage is applied is detected as a change in the intensity of the light depending on the voltage, and this is converted into an electric signal. It measures and processes. Since the measured point is completely electrically separated from the measuring instrument, all the effects of grounding and electrical sneak-up described above are avoided.
【0011】[0011]
【実施例】以下,本発明の実施例について,図面を参照
して説明する。Embodiments of the present invention will be described below with reference to the drawings.
【0012】(実施例1)図1は本発明による電圧波形
の計測するための計測器用プローブの一構成例を示す図
である。また,図2は図1の光変調器の拡大図である。
図1に示すように,計測器用プローブは,二つの検出端
子1,2を備えた導体3,4と,導体3,4に接続さ
れ,容器20内に収容された光変調器5,光源11,光
変調器5の一端と光源11とを接続する光入力部として
入力光ファイバ12,光源11に接続された電源21,
光検出器16,光変調器5の他端と光検出器16とを接
続する光出力部として出力光ファイバ15,オシロスコ
ープ19,及び光検出器16に接続された同軸コネクタ
17を有する同軸ケーブル18を備えている。(Embodiment 1) FIG. 1 is a diagram showing a configuration example of a probe for a measuring instrument for measuring a voltage waveform according to the present invention. 2 is an enlarged view of the optical modulator shown in FIG.
As shown in FIG. 1, the probe for a measuring instrument includes conductors 3 and 4 having two detection terminals 1 and 2, an optical modulator 5 connected to the conductors 3 and 4, and a light source 11 that is housed in a container 20. , An input optical fiber 12 as an optical input section for connecting one end of the optical modulator 5 and the light source 11, a power source 21 connected to the light source 11,
A photodetector 16, a coaxial cable 18 having an output optical fiber 15 as an optical output section for connecting the other end of the optical modulator 5 and the photodetector 16, an oscilloscope 19, and a coaxial connector 17 connected to the photodetector 16. Is equipped with.
【0013】図2に示すように,光変調器5は,電気光
学効果を示すニオブ酸リチウム結晶を基板6とし,その
表面に光導波路9,10が夫々形成され,それぞれの光
導波路9,10の表面を覆うように,一対の電極7,8
が重ねられて形成されている。入力光ファイバ12に接
続され入射光導波路13から分岐して位相シフト光導波
路9,10が形成され,再び出射導波路14に合流し
て,出力光ファイバ15に接続されている。また,一対
の電極には,夫々導体3,4が接続され,マッハツェン
ダ光干渉計を構成している。As shown in FIG. 2, the optical modulator 5 uses a substrate 6 made of lithium niobate crystal exhibiting an electro-optical effect, and optical waveguides 9 and 10 are formed on the surface of the substrate 6, respectively. A pair of electrodes 7, 8 so as to cover the surface of the
Are formed by overlapping. The phase shift optical waveguides 9 and 10 are formed by branching from the incident optical waveguide 13 while being connected to the input optical fiber 12, joined again to the outgoing waveguide 14, and connected to the output optical fiber 15. Further, the conductors 3 and 4 are respectively connected to the pair of electrodes to form a Mach-Zehnder optical interferometer.
【0014】図1及び図2を参照して,二つの検出端子
1,2から入力した被測定信号は,導体3,4によって
光変調器5の電極7,8に導かれる。光源11は半導体
レーザを備え,光ファイバ12によって光変調器5の入
射光導波路13に導かれ,二つの位相シフト光導波路
9,10によって分岐し,電極7,8の近傍を通り,出
射導波路14に合流する。前記検出端子1,2から導か
れた被測定電圧は電極7,8を介して二つの位相シフト
光導波路9,10に電界を発生し,局部的に屈折率の変
化をもたらす。このためこれら二つの位相シフト光導波
路9,10を通る光に位相差が生じ,これらが合流する
出射光導波路14では互いに干渉し,印加される電圧に
依存して強度変化をもつ光となる。光強度の変化は,し
たがって,出力光ファイバ15を介して光検出器16に
よって電気信号に変換され,同軸コネクタ17を有する
同軸ケーブル18,オシロスコープ19等の非対称計測
器に伝送され,計測処理される。Referring to FIGS. 1 and 2, the signals under measurement input from the two detection terminals 1 and 2 are guided to the electrodes 7 and 8 of the optical modulator 5 by the conductors 3 and 4. The light source 11 includes a semiconductor laser, is guided by an optical fiber 12 to an incident optical waveguide 13 of an optical modulator 5, is branched by two phase shift optical waveguides 9 and 10, passes near the electrodes 7 and 8, and is an emission waveguide. Join 14 The voltage to be measured introduced from the detection terminals 1 and 2 generates an electric field in the two phase shift optical waveguides 9 and 10 via the electrodes 7 and 8 and locally causes a change in the refractive index. Therefore, a phase difference occurs in the light passing through these two phase shift optical waveguides 9 and 10, and in the output optical waveguide 14 where these merge, they interfere with each other and become light having an intensity change depending on the applied voltage. Therefore, the change in the light intensity is converted into an electric signal by the photodetector 16 via the output optical fiber 15, and is transmitted to the asymmetrical measuring device such as the coaxial cable 18 having the coaxial connector 17, the oscilloscope 19 and the like and processed. .
【0015】本発明の実施例1において用いた光変調器
5の大きさは,ほぼ長さ50mm,幅3mm,厚さ0.
5mmで,稼動部分がなく,電源を必要としなく,いわ
ゆるメンテナンスフリーである。このため,図1に示す
ように光変調器5を,有機高分子材料の樹脂からなる細
い筒状の容器20に収容したままで計測に供することが
できる。この構成による計測器用プローブと非対称計測
器であるオシロスコープ19を用い,すなわち図1の計
測系の構成によって,高周波回路内の電圧波形の計測を
行い,従来の電気式プローブを使った場合に頻発した種
々の問題は全くなく,十分な信頼をもつ結果を得た。The size of the optical modulator 5 used in the first embodiment of the present invention is approximately 50 mm in length, 3 mm in width, and 0.
It is 5 mm, has no moving parts, does not require a power supply, and is so-called maintenance-free. Therefore, as shown in FIG. 1, the optical modulator 5 can be used for measurement while being housed in a thin cylindrical container 20 made of a resin of an organic polymer material. The voltage probe in the high-frequency circuit was measured by using the measuring instrument probe with this configuration and the oscilloscope 19 which is an asymmetrical measuring instrument, that is, by the configuration of the measuring system in FIG. 1, and frequently occurred when the conventional electric probe was used. There were no problems at all, and the results were sufficiently reliable.
【0016】(実施例2)図3は本発明の実施例2に係
る計測器用プローブの構成を示す図である。図3に示す
計測器用プローブはいわゆる反射型の光変調器を用いて
構成されている。(Embodiment 2) FIG. 3 is a view showing the arrangement of a measuring instrument probe according to Embodiment 2 of the present invention. The measuring instrument probe shown in FIG. 3 is configured using a so-called reflection type optical modulator.
【0017】図3に示すように,計測器用プローブは,
二つの検出端子1,2を備えた導体3,4と,導体3,
4に接続され,容器20内に収容された光変調器25,
光源11,光源11に接続された電源21,光源11に
接続された光サーキュレータ28,光サーキュレータ2
8と光変調器25とを接続する光入出力部である偏波保
持ファイバ12′,光サーキュレータ28に接続された
光検出器16,オシロスコープ19,及び光検出器16
とオシロスコープ19とを接続する同軸コネクタ17を
有する同軸ケーブル18を備えている。実施例2に係る
光変調器25は,実施例1とは構成を異にするが,その
機能および原理において同じである。As shown in FIG. 3, the measuring instrument probe is
Conductors 3 and 4 having two detection terminals 1 and 2, and conductors 3 and 4.
4, an optical modulator 25 housed in a container 20,
Light source 11, power source 21 connected to light source 11, optical circulator 28 connected to light source 11, optical circulator 2
8, a polarization maintaining fiber 12 ', which is an optical input / output unit connecting the optical modulator 25 and the optical modulator 25, a photodetector 16 connected to the optical circulator 28, an oscilloscope 19, and a photodetector
And a coaxial cable 18 having a coaxial connector 17 for connecting the oscilloscope 19 and the oscilloscope 19. The optical modulator 25 according to the second embodiment has a different structure from that of the first embodiment, but has the same function and principle.
【0018】図4は図3に用いた光変調器25を拡大し
て模式的に示した図である。図4に示すように,電気光
学効果の性質を有するニオブ酸リチウム結晶からなる基
板24上に,二つに分岐した位相シフト光導波路22,
23が形成されている。この位相シフト光導波路22,
23の端面には全反射膜26が付設されている。全反射
膜26の存在によって光導波路によるマッハツェンダ光
干渉計が形成されている。光変調器25への入力光およ
び反射による出力光は一本の偏波保持ファイバ12′に
よって伝送される。図3及び図4を参照して,偏波保持
ファイバ12′により,光源11からの入力光と,光変
調器25から光検出器16に導く出力光とは,光方向分
離器として光サーキュレータ28を用いて互いに分離さ
れる。光源11からの光は光サーキュレータ28および
偏波保持ファイバ12′を通じて,容器20内に格納さ
れた光変調器1に入射する。二つの位相シフト光導波路
9,10に分岐した光は,電極7,8の近傍を通り,つ
いで全反射膜26によって反射し,同一光路を取って戻
る。FIG. 4 is an enlarged schematic view of the optical modulator 25 used in FIG. As shown in FIG. 4, on the substrate 24 made of lithium niobate crystal having an electro-optical effect, the phase-shifted optical waveguide 22 branched into two,
23 is formed. This phase shift optical waveguide 22,
A total reflection film 26 is attached to the end face of 23. Due to the presence of the total reflection film 26, a Mach-Zehnder optical interferometer using an optical waveguide is formed. The input light to the optical modulator 25 and the output light by reflection are transmitted by one polarization maintaining fiber 12 '. With reference to FIGS. 3 and 4, the input light from the light source 11 and the output light guided from the optical modulator 25 to the photodetector 16 by the polarization maintaining fiber 12 'serve as an optical circulator 28 as an optical direction separator. Are separated from each other. The light from the light source 11 enters the optical modulator 1 stored in the container 20 through the optical circulator 28 and the polarization maintaining fiber 12 '. The light branched to the two phase shift optical waveguides 9 and 10 passes through the vicinity of the electrodes 7 and 8 and is then reflected by the total reflection film 26, and returns along the same optical path.
【0019】一方,検出端子3から導かれた被測定電圧
は電極7,8を介して二つの位相シフト光導波路22,
23に電界を発生し,局部的な屈折率の変化をもたら
す。このためこれらの位相シフト光導波路22,23を
通る光には,往復の過程で位相差が生じ,これらが合流
する光導波路27では互いに干渉し,印加される電圧に
依存して強度変化をもつ光となる。光強度の変化は,偏
波保持ファイバ12′によって光サーキュレータ28を
経由して,光検出器16によって電気信号に変換され,
同軸ケーブル18によりオシロスコープ19等の非対称
計測器に伝送され,計測処理される。On the other hand, the voltage to be measured introduced from the detection terminal 3 is transmitted through the electrodes 7 and 8 to the two phase shift optical waveguides 22 and
An electric field is generated at 23, causing a local change in the refractive index. Therefore, the light passing through the phase shift optical waveguides 22 and 23 has a phase difference in the reciprocating process, and the optical waveguides 27 where these merge are interfered with each other and have intensity changes depending on the applied voltage. Become light. The change in light intensity is converted into an electric signal by the photodetector 16 via the optical circulator 28 by the polarization maintaining fiber 12 ',
It is transmitted to an asymmetrical measuring device such as an oscilloscope 19 by the coaxial cable 18 and processed.
【0020】本発明の実施例2において用いた光変調器
の大きさは,ほぼ長さ25mm,幅3mm,厚さ0.5
mmである。尚,光変変調器を図3に示すように,有機
高分子材料の樹脂からなる細い筒状の容器20に格納し
たままで使うことができるほか,本発明の実施例2にお
いては,図5に示す変形例のように,検出端子1の一つ
を容器先端に固定し,他の一つは可撓性がある導体(導
線)をもつ検出端子をもつ構成とした計測器用プローブ
を作製し,電圧計測に併せて用いた。また,本発明の実
施例2において光サーキュレータ17の代わりに光方向
性結合器を用いても同様な効果が得られた。The size of the optical modulator used in the second embodiment of the present invention is approximately 25 mm in length, 3 mm in width, and 0.5 in thickness.
mm. In addition, as shown in FIG. 3, the optical modulator / modulator can be used as it is stored in a thin cylindrical container 20 made of a resin of an organic polymer material. As in the modification shown in Fig. 1, one of the detection terminals 1 is fixed to the tip of the container, and the other one has a detection terminal having a flexible conductor (conductor wire). , Also used for voltage measurement. Further, in Example 2 of the present invention, the same effect was obtained by using an optical directional coupler instead of the optical circulator 17.
【0021】実施例2は実施例1に比べて入出力光ファ
イバーが1本であり光変調器の片側のみ接続されるので
取扱い易く,かつ,作製も容易である。さらに,同じ感
度を得るための変調器の長さは1/2となるので,小型
化が可能である。また,同じ感度で比較した場合,電極
容量が1/2となるので,より高速波形の観測が可能と
なる。Compared to the first embodiment, the second embodiment has one input / output optical fiber and is connected to only one side of the optical modulator, so that it is easy to handle and easy to manufacture. Further, since the length of the modulator for obtaining the same sensitivity is halved, the size can be reduced. Further, when compared with the same sensitivity, the electrode capacitance is halved, so that a higher speed waveform can be observed.
【0022】(実施例3)図6は本発明の実施例3に係
る計測器用プローブの構成概要を示す図であり,図7は
図6の光変調器の構成を示す図である。図6に示すよう
に,光変調器30として,印加電圧に依存して複屈折が
変化する性質を利用したポッケルス素子31を使った他
は,実施例1と同様の構成を有する。即ち,図6に示す
ように,計測器用プローブは,二つの検出端子1,2を
備えた導体3,4と,導体3,4に接続され,容器20
内に収容された光変調器30,光源11,光変調器30
の一端と光源11とを接続する入力光ファイバ12,光
源11に接続された電源21,光検出器16,光変調器
30の他端と光検出器16とを接続する出力光ファイバ
15,オシロスコープ19,及び光検出器16に接続さ
れた同軸コネクタ17を有する同軸ケーブル18を備え
ている。(Embodiment 3) FIG. 6 is a diagram showing a schematic configuration of a measuring instrument probe according to a third embodiment of the present invention, and FIG. 7 is a diagram showing a configuration of the optical modulator of FIG. As shown in FIG. 6, the optical modulator 30 has the same configuration as that of the first embodiment except that a Pockels element 31 that utilizes the property that the birefringence changes depending on the applied voltage is used. That is, as shown in FIG. 6, the measuring instrument probe is connected to the conductors 3 and 4 having the two detection terminals 1 and 2, and the conductors 3 and 4, and is connected to the container 20.
Light modulator 30, light source 11, and light modulator 30 housed in
Optical fiber 12 for connecting one end of the light source 11 to the light source 11, a power supply 21 connected to the light source 11, a photodetector 16, an output optical fiber 15 for connecting the other end of the optical modulator 30 to the photodetector 16, an oscilloscope 19, and a coaxial cable 18 having a coaxial connector 17 connected to the photodetector 16.
【0023】図7に示すように,本発明の実施例3に係
る計測器用プローブの光変調器30は,ポッケルス素子
31としてBGO結晶(化学式Bi12GeO20)を用い
ている。こののポッケルス素子31は六面体構造を有
し,対向する二つの面に電極28,29をつけ,他の対
向する二つの光学面には,入射面側には偏光子33を,
出射面側には順に波長板34および検光子35を配置し
ている。As shown in FIG. 7, the optical modulator 30 of the measuring instrument probe according to the third embodiment of the present invention uses a BGO crystal (chemical formula Bi 12 GeO 20 ) as the Pockels element 31. This Pockels element 31 has a hexahedral structure, and has electrodes 28 and 29 on two opposing surfaces, and a polarizer 33 on the incident surface side on the other two opposing optical surfaces.
A wave plate 34 and an analyzer 35 are sequentially arranged on the emission surface side.
【0024】図6及び図7を再び参照して,入力光ファ
イバ12を経由する光源11からの光は,レンズ32に
より収束され偏光子33を通り直線偏光となりポッケル
ス素子31に入射される。ポッケルス素子31を通過し
て楕円偏光となった出射光は,波長板34および検光子
35によって強度変調された直線偏光となる。さらに,
この直線偏光はレンズ36を介して収束され,出力光フ
ァイバ15に入射し,この出力光ファイバ15によって
光検出器16に伝送され,ここで電気信号に変換され,
同軸ケーブル18を通ってオシロスコープ19等の非対
称計測器に伝送され,計測処理される。Referring again to FIGS. 6 and 7, the light from the light source 11 passing through the input optical fiber 12 is converged by the lens 32, passes through the polarizer 33, becomes linearly polarized light, and enters the Pockels element 31. The outgoing light that has passed through the Pockels element 31 and has become elliptically polarized light becomes linearly polarized light that is intensity-modulated by the wave plate 34 and the analyzer 35. further,
This linearly polarized light is converged through the lens 36, is incident on the output optical fiber 15, is transmitted to the photodetector 16 by the output optical fiber 15, and is converted into an electric signal here.
It is transmitted through the coaxial cable 18 to an asymmetrical measuring device such as an oscilloscope 19 and processed.
【0025】尚,本発明の実施例3において,光変調器
30は,樹脂からなる容器20の中にポッケルス素子3
1を含むレンズ34,偏光子32,等の光学素子を構築
して構成されている。In the third embodiment of the present invention, the optical modulator 30 includes the Pockels element 3 in the container 20 made of resin.
It is constructed by constructing optical elements such as a lens 34 including 1 and a polarizer 32.
【0026】[0026]
【発明の効果】以上説明したように,本発明による計測
プローブは,オシロスコープの測定プローブと同様の手
軽さをもって,高周波から低周波領域にわたって十分な
信頼性をもつ計測を可能とする。As described above, the measurement probe according to the present invention enables measurement with sufficient reliability from a high frequency region to a low frequency region, as easily as a measurement probe of an oscilloscope.
【図1】本発明の実施例1に係る計測用プローブの構成
図である。FIG. 1 is a configuration diagram of a measurement probe according to a first embodiment of the present invention.
【図2】図1の光変調器の拡大図である。FIG. 2 is an enlarged view of the optical modulator shown in FIG.
【図3】本発明の実施例2に係る計測用プローブの構成
図である。FIG. 3 is a configuration diagram of a measurement probe according to a second embodiment of the present invention.
【図4】図3の光変調器の拡大図である。FIG. 4 is an enlarged view of the optical modulator of FIG.
【図5】図4に示す光変調器を他の容器に収容した変形
例を示す図である。5 is a diagram showing a modified example in which the optical modulator shown in FIG. 4 is housed in another container.
【図6】本発明の実施例3に係る計測用プローブの構成
図である。FIG. 6 is a configuration diagram of a measurement probe according to a third embodiment of the present invention.
【図7】図5の光変調器の拡大図である。FIG. 7 is an enlarged view of the optical modulator of FIG.
1,2 検出端子 3,4 導体 5,25,30 光変調器 6,24 基板 7,8 電極 9,10 光導波路 11 光源 12′ 偏波保持ファイバ 12 入射光ファイバ 13 入射光導波路 14 出射光導波路 15 出力光ファイバ 16 光検出器 17 同軸コネクタ 18 同軸ケーブル 19 オシロスコープ 20 容器 21 光源用電源 22,23 位相シフト光導波路 26 全反射膜 28 光サーキュレータ 31 ポッケルス素子 32,36 レンズ 33 偏光子 34 波長板 35 検光子 1, 2 Detection terminal 3, 4 Conductor 5, 25, 30 Optical modulator 6, 24 Substrate 7, 8 Electrode 9, 10 Optical waveguide 11 Light source 12 'Polarization maintaining fiber 12 Incident optical fiber 13 Incident optical waveguide 14 Emitting optical waveguide 15 Output optical fiber 16 Photodetector 17 Coaxial connector 18 Coaxial cable 19 Oscilloscope 20 Container 21 Light source power source 22, 23 Phase shift optical waveguide 26 Total reflection film 28 Optical circulator 31 Pockels element 32, 36 Lens 33 Polarizer 34 Wave plate 35 Analyzer
Claims (5)
て前記電極の近傍を通った光の強度を変化させる光変調
器と,前記電極に一端が接続され他端に検出端子を備え
た導体と,光源からの光を前記光変調器に伝搬する光入
力部と,前記光変調器からの光出力を伝搬する光出力部
と,前記光出力部に接続され電気出力を非対称計測器に
接続するための同軸コネクタを持つ光検出器とを備え,
前記検出端子を被測定点である電気回路内の任意の2点
に接触または保持する機能を有することを特徴とする計
測器用プローブ。1. An optical modulator for changing the intensity of light passing through the vicinity of the electrode depending on a voltage applied between the two electrodes, and one end connected to the electrode and a detection terminal at the other end. A conductor, an optical input section for propagating light from a light source to the optical modulator, an optical output section for propagating an optical output from the optical modulator, and an asymmetric measuring instrument for electrical output connected to the optical output section. And a photodetector with a coaxial connector for connection to
A probe for a measuring instrument, which has a function of contacting or holding the detection terminal at any two points in an electric circuit which is a measured point.
二つの電極の近傍を通り,他の端面で反射した後,さき
に入射した前記端面から出射する光の強度が,前記印加
電圧に依存して変化する光変調器と,前記電極に一端が
接続され他端に検出端子を備えた導体と,非対称計測器
に接続するための同軸コネクタを持つ光検出器及び前記
光の光源を夫々付設した光方向性分離器と,前記光方向
性分離器及び前記光変調器間を接続する入力及び出力伝
達機能をもつ光伝搬部とを備え,前記検出端子を被測定
点である電気回路内の任意の2点に接触または保持する
機能を有することを特徴とする計測器用プローブ。2. The intensity of light which is incident from one end face, passes through the vicinity of two electrodes to which a voltage is applied, is reflected by the other end face, and then is emitted from the end face which is incident on the other end face is equal to the applied voltage. An optical modulator that changes depending on the light source, a conductor having one end connected to the electrode and a detection terminal at the other end, a photodetector having a coaxial connector for connecting to the asymmetric measuring instrument, and the light source for the light, respectively. In an electric circuit having an attached optical directional separator and an optical propagation section having an input and output transmission function for connecting between the optical directional separator and the optical modulator, and having the detection terminal as a point to be measured. A probe for a measuring instrument, which has a function of contacting or holding any two points of
において,前記光変調器は,非金属材料からなる容器に
収容されていることを特徴とする計測器用プローブ。3. The measuring instrument probe according to claim 1 or 2, wherein the optical modulator is housed in a container made of a non-metallic material.
の計測器用プローブにおいて,前記光変調器はマッハツ
ェンダ光干渉型光変調器であることを特徴とする計測器
用プローブ。4. The measuring instrument probe according to claim 1, wherein the optical modulator is a Mach-Zehnder interferometric optical modulator.
し,該電極の近傍を通り,前記電圧に依存して変化した
光の強度を電気信号に変換した上で,非対称計測器を用
いて計測することを特徴とする電圧計測方法。5. A voltage to be measured is applied to an electrode of an optical modulator, the intensity of light passing through the vicinity of the electrode and changed depending on the voltage is converted into an electric signal, and then an asymmetric measuring device is used. A voltage measuring method characterized by using and measuring.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17065894A JPH0835998A (en) | 1994-07-22 | 1994-07-22 | Measuring instrument probe and voltage measuring method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17065894A JPH0835998A (en) | 1994-07-22 | 1994-07-22 | Measuring instrument probe and voltage measuring method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0835998A true JPH0835998A (en) | 1996-02-06 |
Family
ID=15908972
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17065894A Pending JPH0835998A (en) | 1994-07-22 | 1994-07-22 | Measuring instrument probe and voltage measuring method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0835998A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US11994539B2 (en) | 2020-04-07 | 2024-05-28 | Seikoh Giken Co., Ltd. | Optical voltage probe |
-
1994
- 1994-07-22 JP JP17065894A patent/JPH0835998A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US11994539B2 (en) | 2020-04-07 | 2024-05-28 | Seikoh Giken Co., Ltd. | Optical voltage probe |
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