JPH0140313B2 - - Google Patents
Info
- Publication number
- JPH0140313B2 JPH0140313B2 JP55175453A JP17545380A JPH0140313B2 JP H0140313 B2 JPH0140313 B2 JP H0140313B2 JP 55175453 A JP55175453 A JP 55175453A JP 17545380 A JP17545380 A JP 17545380A JP H0140313 B2 JPH0140313 B2 JP H0140313B2
- Authority
- JP
- Japan
- Prior art keywords
- bso
- optical
- voltage sensor
- bgo
- optical 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.)
- Expired
Links
- 230000003287 optical effect Effects 0.000 claims description 18
- 239000013078 crystal Substances 0.000 claims description 9
- ORCSMBGZHYTXOV-UHFFFAOYSA-N bismuth;germanium;dodecahydrate Chemical compound O.O.O.O.O.O.O.O.O.O.O.O.[Ge].[Ge].[Ge].[Bi].[Bi].[Bi].[Bi] ORCSMBGZHYTXOV-UHFFFAOYSA-N 0.000 claims description 2
- JSILWGOAJSWOGY-UHFFFAOYSA-N bismuth;oxosilicon Chemical compound [Bi].[Si]=O JSILWGOAJSWOGY-UHFFFAOYSA-N 0.000 claims description 2
- 230000035945 sensitivity Effects 0.000 description 7
- 238000010586 diagram Methods 0.000 description 6
- 230000005484 gravity Effects 0.000 description 3
- 239000013307 optical fiber Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R15/00—Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
- G01R15/14—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
- G01R15/24—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices
- G01R15/241—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using electro-optical modulators, e.g. electro-absorption
- G01R15/242—Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using electro-optical modulators, e.g. electro-absorption based on the Pockels effect, i.e. linear electro-optic effect
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Description
本発明はビスマスシリコンオキサイドBSO(以
下BSOという)あるいはビスマスゲルマニウム
オキサイドBGO(以下BGOという)素子を用い
た、広帯域化した光応用電圧センサに関する。
第1図は基本的な光応用電圧センサの構成を示
す図である。1は光フアイバ、2はロツドレン
ズ、3は偏光子、4は1/4波長板、5はBSO素子
あるいはBGO素子、6は検光子、7は入力電圧
源である。BSO素子及びBGO素子共に同じ説明
が適用できるので、以下にはBSO素子を用いて
説明する。光フアイバ1に入射されロツドレンズ
2、偏光子3及び1/4波長板4を通つてBSO素子
5に入射した光は、入力電圧源7から電極を介し
てBSO素子5に印加される電圧の大きさに応じ
て偏光の状態が変わる。光応用電圧センサはこの
偏光の状態を知ることにより被検出入力電圧の大
きさを検出するものである。
第2図は第1図の光応用電圧センサの変調感度
の従来の周波数特性を示す図である。従来の
BSO素子を用いた光応用電圧センサにおいては、
入力電圧の周波数を変えてゆくとある特定周波数
で圧電現象によりBSO素子に機械的共振現象が
発生する。この共振による機械的な応力が更に
BSO素子の屈折率に影響を及ぼす。このため、
従来のBSO素子を用いた光応用電圧センサの変
調感度の周波数特性は第2図に示す様に特定周波
数で非常に大きなピークa,b,c等を発生する
欠点がある。従つて、高電圧のサージ現象等の高
い周波数成分まで一定の変調感度を必要とする解
折には、従来の光応用電圧センサは使用できない
欠点があつた。
本発明の目的は、共振現象の影響をなくし広帯
域化できるBSO素子を用いた光応用電圧センサ
を提供することである。
以下に図面を参照して本発明について詳細に説
明する。
第3図イはBSO素子の形状(長さl×幅w×
厚さb)と方位との関係を示す図である。l×w
面内にx軸、y軸を図のようにとり、l×w面と
垂直につまり厚さbと平行にz軸をとるものとす
る。まず、圧電現象によりBSO素子に前記共振
現象が生ずる理由について発明者が行なつた解析
について説明する。BSOは点群23に属する単
結晶であり、その電気、光学、機械的特性は例え
ば「結晶物理工学」(小川智哉著、裳華房)に詳
述されている。一般的に、BSOの圧電効果は下
記の圧電基本式(テンソル方程式)により記述さ
れる。
Tn=ConSo−ejnEj
Di=eioSo+εijEj …(1)
ここで、Tn:応力、Con:弾性ステイツフネ
ス、So:歪み、ejn、eio:圧電e定数、Ej:印加
電圧、Di:電束密度、εij:誘電率である。第3図
イの系でBSOを使用した場合に、その圧電基本
式は次のようになる。
T1=C11S1+C12S2+C12S3
T2=C12S1+C11S2+C12S3
T3=C12S1+C12S2+C11S3
T4=C44S4
T5=C44S5
T6=C44S6−e14E3
D1=e14S4
D2=e14S5
D3=e14S6+ε11E3 …(2)
(2)式において、BSOに電圧を印加することに
より直接的な影響を受けるのはE3を含むT6及び
D3である。ここで、
T6=T12+T21
=(第2面に働く第1方向の応力)
+(第1面に働く第2方向の応力)
であるから、結局、電圧を印加するとBSOには
せん断応力(shear stress)が作用することにな
る。
結晶を構成する粒子のxi方向への変位をξiとす
ると運動方程式は次のようになる。
ρδ2ξi/δt2=δTij/δxj
ρ:比重
すなわち、
(2)式により
T12=C44S12−e14E3
T21=C44S21−e14E3
更に、S12=S211/2(δξ1/δx2+δξ2/δx1)
であるから、結局、(3)式は
となる。(4)式の解は
ξ1=ξ01ejwtsin(γx2+θ2)
ξ2=ξ02ejwtsin(γx1+θ1) …(5)
但し、
The present invention relates to a broadband optical voltage sensor using a bismuth silicon oxide BSO (hereinafter referred to as BSO) or bismuth germanium oxide BGO (hereinafter referred to as BGO) element. FIG. 1 is a diagram showing the configuration of a basic optical voltage sensor. 1 is an optical fiber, 2 is a rod lens, 3 is a polarizer, 4 is a quarter-wave plate, 5 is a BSO element or BGO element, 6 is an analyzer, and 7 is an input voltage source. Since the same explanation can be applied to both the BSO element and the BGO element, the following explanation will be made using the BSO element. The light that enters the optical fiber 1, passes through the rod lens 2, the polarizer 3, and the 1/4 wavelength plate 4, and enters the BSO element 5 depends on the magnitude of the voltage applied from the input voltage source 7 to the BSO element 5 via the electrodes. The state of polarization changes depending on the The optical voltage sensor detects the magnitude of the input voltage to be detected by knowing the state of this polarization. FIG. 2 is a diagram showing the conventional frequency characteristics of modulation sensitivity of the optical voltage sensor shown in FIG. Traditional
In optical voltage sensors using BSO elements,
As the frequency of the input voltage is changed, a mechanical resonance phenomenon occurs in the BSO element due to the piezoelectric phenomenon at a certain frequency. The mechanical stress caused by this resonance is further
Affects the refractive index of the BSO element. For this reason,
As shown in FIG. 2, the frequency characteristics of the modulation sensitivity of a conventional optical voltage sensor using a BSO element has the drawback of generating very large peaks a, b, c, etc. at specific frequencies. Therefore, conventional optical voltage sensors cannot be used for analysis that requires constant modulation sensitivity up to high frequency components such as high voltage surge phenomena. An object of the present invention is to provide an optical voltage sensor using a BSO element that can eliminate the influence of resonance phenomena and achieve a wide band. The present invention will be described in detail below with reference to the drawings. Figure 3 A shows the shape of the BSO element (length l x width w x
It is a figure showing the relationship between thickness b) and orientation. l×w
Assume that the x-axis and y-axis are taken in the plane as shown in the figure, and the z-axis is taken perpendicular to the l×w plane, that is, parallel to the thickness b. First, an analysis conducted by the inventor regarding the reason why the resonance phenomenon occurs in the BSO element due to the piezoelectric phenomenon will be explained. BSO is a single crystal belonging to point group 23, and its electrical, optical, and mechanical properties are detailed in, for example, "Crystal Physics Engineering" (written by Tomoya Ogawa, published by Shokabo). Generally, the piezoelectric effect of BSO is described by the piezoelectric basic equation (tensor equation) below. T n = C on S o −e jn E j D i = e io S o +ε ij E j …(1) Here, T n : Stress, C on : Elastic state funes, S o : Strain, e jn , e io : piezoelectric e constant, E j : applied voltage, D i : electric flux density, ε ij : permittivity. When BSO is used in the system shown in Figure 3A, the basic piezoelectric formula is as follows. T 1 = C 11 S 1 + C 12 S 2 + C 12 S 3 T 2 = C 12 S 1 + C 11 S 2 + C 12 S 3 T 3 = C 12 S 1 + C 12 S 2 + C 11 S 3 T 4 = C 44 S 4 T 5 = C 44 S 5 T 6 = C 44 S 6 −e 14 E 3 D 1 = e 14 S 4 D 2 = e 14 S 5 D 3 = e 14 S 6 +ε 11 E 3 …(2) In equation (2), T 6 including E 3 and T 6 are directly affected by applying voltage to BSO.
D3 . Here, T 6 = T 12 + T 21 = (stress in the first direction acting on the second surface) + (stress in the second direction acting on the first surface), so in the end, when a voltage is applied, shear is applied to the BSO. Stress (shear stress) will act. Letting ξ i be the displacement of the particles constituting the crystal in the x i direction, the equation of motion is as follows. ρδ 2 ξ i / δt 2 = δT ij / δx j ρ: Specific gravity, that is, According to equation (2), T 12 = C 44 S 12 −e 14 E 3 T 21 = C 44 S 21 −e 14 E 3 Furthermore, S 12 = S 21 1/2 (δξ 1 / δx 2 + δξ 2 / δx 1 ), so in the end, equation (3) becomes becomes. The solution to equation (4) is ξ 1 = ξ 01 e jwt sin (γx 2 + θ 2 ) ξ 2 = ξ 02 e jwt sin (γx 1 + θ 1 ) …(5) However,
【式】γ=w/v、ξ01、ξ02は定数
である。これは第3図ロに実線及び点線で示すい
わゆる面すべり振動(face shear mode)であ
る。以上まとめると、第3図イの座標系でBSO
を使用した場合、結晶に発生する圧電現象はx軸
−y軸平面において生ずる面すべり振動であり、
z軸方向の厚みbにはほとんど依存しないことが
わかつた。
面すべり振動における共振周波数Rは近似的に
次式で与えられることが知られている。
この共振周波数は基本モード(m=n=1)に
おいては
で示される。ここで、ρ:比重、C44:圧電ステ
イツフネス、l及びw:BSO素子の長さ及び幅。
BSOの場合、圧電ステイツフネスC44=0.25×
10″(N/m2)、比重ρ=9.2×103(Kg/m3)程度で
ある。BSO素子の大きさに対する共振周波数に
ついての発明者の行なつた実験結果と計算結果と
を表1に示す。[Formula] γ=w/v, ξ 01 and ξ 02 are constants. This is the so-called face shear mode shown by solid lines and dotted lines in FIG. To summarize the above, in the coordinate system of Figure 3 A, BSO
When using , the piezoelectric phenomenon that occurs in the crystal is a plane shear vibration that occurs in the x-axis-y-axis plane,
It was found that there is almost no dependence on the thickness b in the z-axis direction. It is known that the resonance frequency R in plane slip vibration is approximately given by the following equation. In the fundamental mode (m=n=1), this resonant frequency is It is indicated by. Here, ρ: specific gravity, C 44 : piezoelectric states funes, l and w: length and width of the BSO element.
For BSO, piezoelectric states funes C 44 = 0.25×
10'' (N/m 2 ), specific gravity ρ = about 9.2×10 3 (Kg/m 3 ).The inventor's experimental results and calculation results regarding the resonant frequency with respect to the size of the BSO element are shown below. Shown in 1.
【表】
この表1から分かる様に、実験値は計算値の
0.85倍程度になつており比較的良く一致してい
る。また、BSO素子のlとwとが同じでbのみ
が異なる(1)の7×5×2のBSO素子と(4)の7×
5×1のBSO素子では共振周波数が殆んど変化
しないことがわかる。
第4図イは本発明のBSO素子を用いた光応用
電圧センサの変調感度の周波数特性を例示する図
である。前述した発明者の解析及び実験により、
BSOの結晶をZカツトとし光をZ方向に通すこ
とによりかなり面すべり振動の影響を避けること
ができ、従つてかなりの高周波成分まで光応用電
圧センサの変調感度のピークをなくすことができ
ることがわかつた。高電圧応用分野では立ち上が
り時間1μsec立ち下がり時間40μsecのいわゆる標
準インパルス波形が多用されるが、本センサで標
準インパルス波形を測定するためには共振周波数
が少なくとも500KHz以上である必要がある。発
明者は500KHz以上の高共振周波数を有する光応
用電圧センサを得るために、BSOの結晶をZカ
ツトとし光をZ方向に通し、結晶の大きさを光が
通る方向に垂直な面内でl×wとするとき(7)式に
おいて[Table] As can be seen from Table 1, the experimental values are lower than the calculated values.
It is about 0.85 times, which is a relatively good agreement. In addition, the 7×5×2 BSO element in (1) where l and w are the same and only b differs, and the 7×
It can be seen that the resonant frequency hardly changes in the 5×1 BSO element. FIG. 4A is a diagram illustrating the frequency characteristics of modulation sensitivity of an optical voltage sensor using the BSO element of the present invention. Through the inventor's analysis and experiments mentioned above,
It was found that by using a Z-cut BSO crystal and transmitting light in the Z direction, the effects of plane-slip vibration can be avoided to a large extent, and therefore, the peak of modulation sensitivity of optical voltage sensors can be eliminated up to considerably high frequency components. Ta. In the field of high voltage applications, a so-called standard impulse waveform with a rise time of 1 μsec and a fall time of 40 μsec is often used, but in order to measure the standard impulse waveform with this sensor, the resonant frequency must be at least 500 KHz or higher. In order to obtain an optical voltage sensor with a high resonant frequency of 500KHz or more, the inventor used a BSO crystal as a Z-cut to pass light in the Z direction, and changed the size of the crystal to l in a plane perpendicular to the direction in which the light passes. When ×w, in equation (7),
【式】となるよう
に設定すればよいことを提案するものである。ま
た、第4図イの例えば500KHz以上の高周波数に
おける共振現象は第4図ロに示す特性のフイルタ
を使用して光の受信機部分の信号帯域を制限する
ことにより取り去ることができる。このようにし
て得られたBSO素子を第1図の光応用電圧セン
サのBSO素子5として用いることにより、セン
サの周波数特性が改善され広帯域化ができるもの
である。It is proposed that it should be set so that [Formula] is satisfied. Further, the resonance phenomenon at a high frequency of 500 KHz or higher, for example, shown in FIG. 4A can be removed by limiting the signal band of the optical receiver section using a filter having the characteristics shown in FIG. 4B. By using the BSO element thus obtained as the BSO element 5 of the optical voltage sensor shown in FIG. 1, the frequency characteristics of the sensor can be improved and the frequency band can be increased.
第1図は基本的な光応用電圧センサの構成を示
す図、第2図は第1図のセンサの変調感度の従来
の周波数特性を示す図、第3図イはBSO素子の
形状と方位との関係を示す図、ロは面すべり振動
を示す図、第4図イは本発明のBSO素子を用い
た光応用電圧センサの変調感度の周波数特性を例
示する図、ロはフイルタの特性を示す図である。
1:光フアイバ、2:ロツドレンズ、3:偏光
子、4:1/4波長板、5:BSO素子あるいはBGO
素子、6:検光子、7:入力電圧源、a,b,
c:ピーク値、l×w×b:素子の長さ×幅×厚
さ。
Figure 1 shows the configuration of a basic optical voltage sensor, Figure 2 shows the conventional frequency characteristics of the modulation sensitivity of the sensor in Figure 1, and Figure 3A shows the shape and orientation of the BSO element. Figure 4A is a diagram illustrating the frequency characteristics of the modulation sensitivity of an optical voltage sensor using the BSO element of the present invention, Figure 4B is a diagram showing the characteristics of the filter. It is a diagram. 1: Optical fiber, 2: Rod lens, 3: Polarizer, 4: 1/4 wavelength plate, 5: BSO element or BGO
Element, 6: Analyzer, 7: Input voltage source, a, b,
c: peak value, l x w x b: length x width x thickness of element.
Claims (1)
ビスマスゲルマニウムオキサイドBGO単結晶に
印加される電圧を検出する光応用電圧センサにお
いて、BSOあるいはBGO単結晶がZカツトされ
そのサイズがZ方向に垂直な面内で長さl×幅w
(mm)とする時 となるようにされ、光をZ方向に通すように
BSOあるいはBGO素子を構成したことを特徴と
する光応用電圧センサ。[Claims] 1. In an optical voltage sensor that detects a voltage applied to a bismuth silicon oxide BSO or bismuth germanium oxide BGO single crystal, the BSO or BGO single crystal is Z-cut and its size is in a plane perpendicular to the Z direction. Length l x width w within
(mm) so that the light passes in the Z direction.
An optical voltage sensor characterized by comprising a BSO or BGO element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55175453A JPS5798863A (en) | 1980-12-12 | 1980-12-12 | Voltage sensor under photo application |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55175453A JPS5798863A (en) | 1980-12-12 | 1980-12-12 | Voltage sensor under photo application |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5798863A JPS5798863A (en) | 1982-06-19 |
| JPH0140313B2 true JPH0140313B2 (en) | 1989-08-28 |
Family
ID=15996331
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55175453A Granted JPS5798863A (en) | 1980-12-12 | 1980-12-12 | Voltage sensor under photo application |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5798863A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58196359A (en) * | 1982-05-12 | 1983-11-15 | Nissan Motor Co Ltd | Lock-up torque converter |
| CN103809012A (en) * | 2014-02-19 | 2014-05-21 | 广西电网公司电力科学研究院 | Synchronous output apparatus for voltage wave signal based on optical electric field transducer |
-
1980
- 1980-12-12 JP JP55175453A patent/JPS5798863A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5798863A (en) | 1982-06-19 |
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